<<

kChapter 3

DAVID M. CRUDEN AND DAVIDJ. VARNES TYP AND PROCESSES

iN I it.iuiir.iij Words strain, Crack and sometimes break, under burden, range of landslide processes is reviewed in Under the , slip, slide, perish, T this chapter, and vocabulary is provided for Decay with imprecision, will not stay in place, describing the features of relevant Will not stay still. . to their classification for avoidance, control, or re- mediation. The classification of landslides in the Such displaced terms are identified in this chapter. previous landslide report (Vames 1978) has been Following Vames (1978), the use of terms relating widely adopted,, so departures from it have been to the geologic, geomorphic, geographic, or cli- minimized and the emphasis is on the progress made matic characteristics of a landslide has been dis- since 1978. Although this chapter is complete in couraged, and the section in the previous report in itself, particular attention is drawn to changes and which these terms are discussed has been deleted. additions to the vocabulary used by Vames in the The viewpoint of the chapter is that of the previous report and the reasons for the changes. investigator responding to a report of a landslide The term landslide denotes "the movement of on a transportation route. What can usefully a of , or down a slope" observed and how should these observations be (Cruden 1991, 27). The phenomena described as succinctly and unambiguously described? landslides are not limited either to the or to The technical literature describing landslides ; the word as it is now used in North has grown considerably since 1978. An important America has a much more extensive meaning than source of landslide information is the proceedings its component parts suggest (Cruden 1991). The of the International Symposium on Landslides. coverage in this chapter will, however, be identi- The third symposium met in New Delhi, cal to that of the previous report (Vames 1978). (Swaminathan 1980), and the symposium has since Ground and collapse are excluded, and met quádriennially in Toronto, (Canadian and falls are not discussed. Geotechnical Society 1984); in Lausanne, Switzer- This chapter also follows Vames' expressed land (Bonnard 1988); and in Christchurch, New intention of (1978, 12) "developing and attempting Zealand (Bell 1992); it is scheduled to meet in to make more precise a useful vocabulary of terms Trondheim, , in 1996. by which... [landslides] ... may be described." The Among the other important English language terms Vames recommended in 1978 are largely texts and collections of descriptions of landslides retained unchanged and a few useful new terms have been those by Zaruba and Mend (1982), have been added. Eliot (1963, 194) noted: Brunsden and Prior (1984), Crozier (1986), and

36 Landslide Types and Processes 37

Costa and Wieczorek (1987). Eisbacher and with landslide activity, many of Hutchinson's sug- Clague (1984) and Skermer's translation of Heim's gestions from the Working Party on the World Bergsturz und Men.schenleben (1932) have made Landslide Inventory (WP/WLI) have been descriptions of the classic landslides of the Euro- adopted (WP/WLI 1993a,b). pean more accessible to North Americans. Under Hutchinson's chairmanship, the Interna- Important reviews of landsliding around the tional Association of (IAEG) world were edited by Brabb and Harrod (1989) and Commission on Landslides and Other Mass Move- Kozlovskii (1988). Kyunttsel (1988) reviewed ments continued its on terminology. The experience with classification in the USSR and declaration by the United Nations of the Inter- noted "considerable divergences of views between national Decade for Natural Reduction various researchers concerning the mechanisms (1990-2000) prompted the IAEG Commission's underlying certain types of landslides. This applies Suggested Nomenclature for Landslides (1990) and particularly to lateral spreads." the creation of the WP/WLI by the International A historical perspective has been added to the Geotechnical Societies and the United Nations discussion of spreading to show that this type of Educational, Scientific, and Cultural Organization landslide was recognized in over (UNESCO). The Working Party, formed from the 100 years ago and is represented here by some IAEG Commission, the Technical Committee on extremely large movements. Both the size and the Landslides of the International Society for gentle slopes of these movements command par- and Engineering, and nom- ticular attention. inees of the International Society for Rock Me- Crozier commented: chanics, published Directory of the World Landslide Inventory (Brown et al. 1992) listing many workers The two generalized classifications most likely interested in the description of landslides world- to be encountered in the English speaking wide. The Working Party has also prepared the world are by J .N. Hutchinson (1968; Skempton Multilingual Landslide Glossary, which will encour- and Hutchinson, 1969) and D.J. Vames (1958; age the use of standard terminology in describing 1978). . . . Both authors use type of movement landslides (WP/WLI 1993b). The terminology to establish the principal groups.. . . The major suggested in this chapter is consistent with the sug- distinction between the two classifications is gested methods and the glossary of the UNESCO the difference accorded to the status of flow Working Party (WP/WLI 1990, 1991, 1993a,b). movements . . . slope movements which are initiated by shear failure on distinct, boundary shear surfaces but which subsequently achieve 2.FORMING NAMES most of their translational movement by The criteria used in the classification of landslides flowage... this dilemma depends on whether presented here follow Varnes (1978) in emphasiz- the principal interest rests with analyzing the ing type of movement and type of material. Any conditions of failure or with treating the results landslide can be classified and described by two of movement. Hutchinson's classification nouns: the first describes the material and the sec- appears to be related more closely to this first purpose. . . . Both Hutchinson's and Vames' ond describes the type of movement, as shown in classifications have tended to converge over 3-1 (.g., rock fall, ). recent years, particularly in terminology. The names for the types of materials are un- Whereas Vames' scheme is perhaps easier changed from Varnes's classification (1978): rock, to apply and requires less expertise to use, debris, and earth. The definitions for these terms are Hutchinson's classification has particular given in Section 7. Movements have again been appeal to the engineer contemplating stability divided into five types: falls, topples, slides, spreads, analysis. (Crozier 1986, Ch. 2) and flows, defined and described in Section 8. The sixth type proposed by Varnes (1978, Figure 2.2), The synthesis of these two classifications has con- complex landslides, has been dropped from the for- tinued. Hutchinson (1988) included topples, and mal classification, although the term complex has this chapter has benefited from his comments. In been retained as a description of the style of activ- Section 4 of this chapter particularly, which deals ity of a landslide. Complexity can also be indicated 38 Landslides: Investigation and Mitigation

Table 3-1 Abbreviated Classification of Slope Movements

TYPE OF MATERIAL TYPE OF ENGINEERING MOVEMENT PREDOMINANTLY COARSE PREDOMINANTLY FINE Fall Rock fall Debris fall Earth fall Topple Rock topple Debris topple Earth topple Slide Rock slide Debris slide Earth slide Spread Rock spread Debris spread Earth spread Flow Rock flow Debris flow Earth flow

by combining the five types of landslide in the ways The name of a landslide can become moreelab- suggested below. The large classification chart orate as more information about the movement accompanying the previous report (Vames 1978, becomes available. To build up the complete iden- Figure 2.1) has been divided into separate figures tification of the movement, descriptors are added distributed throughout this chapter. in front of the two-noun classification using a pre- ferred sequence of terms. The suggested sequence Table 3-2 provides a progressive narrowing of the focus of the Glossary for Forming Names of Landslides descriptors, first by and then by spatial loca- AcnvrrY tion, beginning with a view of the whole landslide, STATE DISTRIBUTION S1mE continuing with parts of the movement, and finally defining the materials involved: The recommended Active Advancing complex sequence, as shown in Table 3-2, describes activity Reactivated Retrogressive Composite Suspended Widening Multiple (including state, distribution, and style) followed Inactive Enlarging Successive by descriptions of all movements (including rate, Dormant Confined Single content, material, and type). Abandoned Diminishing This sequence is followed throughout the chap- Stabilized Moving ter and all terms given in Table 3-2 are highlighted Relict in bold type and discussed. Second or subsequent DESCRIPTION OF FIRST MOVEMENT movements in complex or composite landslides can be described by repeating, as many as RATE MATERIAL TYPE necessary, the descriptors used in Table 3-2. Extremely rapid Dry Rock Fall Descriptors that are the same as those for the first Very rapid Moist Soil Topple movement may then be dropped from the name. Rapid Wet Earth Slide For instance, the very large and rapid slope Moderate Very wet Debris Spread movement that occurred near the town of Frank, Slow Flow Very slow , Canada, in 1903 (McConnell and Brock Extremely slow 1904) was a complex, extremely rapid, dry rock fall—debris flow (Figure 3-1). From the full name of DESCRIPTION OF SECOND MOVEMENT this landslide at Frank, one would know that both RATE WATER CONTENT MATERIAL TYPE the debris flow and the rock fall were extremly rapid and dry because no other descriptors are used Extremely rapid Dry Rock Fall for the debris flow. Very rapid Moist Soil Topple Rapid Wet Earth Slide As discussed in Section 4.3, the addition of the Moderate Very wet Debris Spread descriptor complex to the name indicates the Slow Flow sequence of movement in the landslide and dis- Very slow tinguishes this landslide from a composite rock Extremely slow fall—debris flow, in which rock fall and debris flow NoTE: Subsequent movements may be described by repeating the above descriptors as movements were occurring, sometimes simultane- many times as necessary. ously, on different parts of the displaced mass. The Landslide Types and Processes 39

FIGURE 3-1 Slide at Frank, Alberta, Canada (oblique aerial photograph from south). About 4:10 am. on April 29, 1903, about 85 million tonnes of rock moved down n. 'i•' east face of Turtle , across entrance of Frank

.t-., .,. mine of Canadian American Company, Crowsnest , southern end of town of Frank, main from east, and Canadian Pacific mainline through . Displaced mass continued up opposite side of valley before coming to rest 120 m above valley floor. Event lasted about 100 seconds. N-IOTOGRAPII NAL'LT3IL. I A Rt1K0I lilt hI I I-IC IM COI.LECTION NATIONAL AIR PlIOTO LIBRARY WITH rERI.IISSION or NATURAL RESOURCES CANADA

full name of the landslide need only be given once; among , to establish type examples with subsequent references should then be to the initial which other landslides may be compared. Shreve material and type of movement, for example, "the (1968), for instance, referred to the landslide in rock fall" or "the Frank rock fall" for the landslide Frank, Alberta, as belonging to the Blackhawk type. at Frank, Alberta. It seems clear that type examples should be historic Several noun combinations may be required to landslides that have been investigated in detail identify the multiple types of material and move- shortly after their occurrence and are of continu- ment involved in a complex or composite land- ing interest to landslide specialists. In addition, for slide. To provide clarity in the description, a dash a type example to be useful, other landslides with known as an " dash" is used to link these stages, the same descriptors should occur in similar mate- as in rock fall—debris flow in the example above. rial. The Blackhawk landslide (Figure 3-2) was a (An en dash is half the length of a re(:,ular dash and prehistoric landslide, and thus was not subject to longer than a hyphen; it is used to remove ambi- investigation at its occurrence (Shreve 1968). It is guity by indicating linkages between terms com- therefore not a suitable type example; neverthe- posed of two nouns.) less, it may have been a Frank-type landslide. The full name of a landslide may be ciimber- Although Vames (1978, 25) discussed "terms some and there is a natural tendency, particularly relating to geologic, geomorphic, geographic, or 40 Landslides: Investigation and Mitigation

tions may be unlikely. The inclusion of complex and composite landslides would increase the num- ber of type examples to over a billion.

3. LANDSLIDE FEATURES AND GEOMETRY

l3e!uie landslide lypes ale discussed, it is uscful to - • '4. establish a nomenclattir&. It r ii it vil tir liii RI- slide features and to discuss the methods of express- ing the dimensions and geometry of landslides.

3.1 Landslide Features

Varnes (1978, Figure 2.1t) provided an idealized diagram showing the features for a complex earth slide—earth flow, which has been reproduced here as Figure 3-3. More recently, the IAEG Commission on Landslides (1990) produced a new idealized landslide diagram (Figure 3-4) in which the van- otis features are identified by numbers, which are defined in different languages by referring to the accompanying tables. Table 3-3 provides the defi- FIGURE 3-2 climatic setting," he recommended against the nitions in English. Blackhawk landslide practice of using type examples because the terms The names of the features are unchanged from view upslope to "are not informative to a reader who lacks knowl- Varnes's classification (1978). However, Table south over lobe of dark edge of the locality" (1978, 26). Moreover, type 3-3 contains explicit definitions for the surface of spread examples are impractical because of the sheer rupture (Figure 3-4, 10), the depletion (16), the beyond mouth of number required to provide a fairly complete land- depleted mass (17), and the accumulation (18) and Blackhawk Canyon slide classification. About 100,000 type examples expanded definitions for the surface of separation on north slope of would be required for all the combinations of (12) and the flank (19). The sequence of the first San Bernardino descriptors and materials with all the types of nine landslide features has been rearranged to pro- in movement defined in Table 3-2 and in the follow- ceed from the crown above the head of the dis- southern . ing sections, although admittedly some combina- Maximum width of placed material to the toe at the foot of the lobe is 2 to 3 km; height of scarp at near edge is about 15 m [Varnes 1978, Figure 2.28 (Shelton 1966)]. COPYRIUI IT Jot IN S. SHELTON

FIGURE 3-3 Block diagram of idealized complex earth slide—earth flow (Varnes 1978, Figure 2.1t). Landslide Types and Processes 41 displaced material. This sequence may make these FIGURE 3-4 Landslide features: features easier to remember. upper portion, plan It may also be helpful to point Out that in the of typical landslide zone of depletion (14) the of the ground in which dashed line surface decreases as a result of landsliding, whereas indicates trace of in the zone of accumulation (15) the elevation of rupture surface on the ground surface increases. If topographic original ground or digital models of the landslide exist for surface; lower both before and after movements, the zones of portion, section in which hatching depletion and accumulation can be found from the indicates undisturbed differences between the maps or models. The vol- ground and stippling ume decrease over the zone of depletion is, of shows extent of course, the depletion, and the volume increase displaced material. over the zone of accumulation is the accumula- Numbers refer to tion. The accumulation can be expected to be features defined in larger than the depletion because the ground gen- Table 3-3 (IAEG erally dilates during landsliding. Commission on Landslides 1990). Table 3-3 Definitions of Landslide Features

NUMBER NAME DEFINITION 1 Crown Practically undisplaced material adjacent to highest parts of main scarp 2 Main scam Steep surface on undisturbed ground at upper edge of landslide caused by movement of displaced material (13, stippled area) away from undisturbed ground; it is visible part of surface of rupture (10) 3 Highest point of contact between displaced material (13) and main scarp(2) (2) 4 Head Upper parts of landslide along contact between displaced material and main scam 5 Minor scam Steep surface on displaced material of landslide produced by differential movements within displaced material 6 Main body Part of displaced material of landslide that overlies surface of rupture between main scam (2) and toe of surface of rupture (II) 7 Foot Portion of landslide that has moved beyond toe of surface of rupture (11) and overlies original ground surface (20) 8 Tip Point on toe (9) farthest from top (3) of landslide 9 Toe Lower, usually curved margin of displaced material of a landslide, most distant from main scarp(2) 10 Surface of rupture Surface that forms (or that has formed) lower boundary of displaced material (13) below original ground surface (20); mechanical idealization of surface of rupture is called slip surface in Chapter 13 11 Toe of surface of (usually buried) between lower part of surface of rupture (10) of a landslide rupture and original ground surface (20) 12 Surface of separation Part of original ground surface (20) now overlain by foot (7) of landslide 13 Displaced material Material displaced from its original position on slope by movement in landslide; forms both depleted mass (17) and accumulation (18); it is stippled in Figure 3-4 14 Zone of depletion Area of landslide within which displaced material (13) lies below original ground surface (20) 15 Zone of accumulation Area of landslide within which displaced material lies above original ground surface (20) 16 Depletion Volume bounded by main scam (2), depleted mass (17), and original ground surface (20) 17 Depleted mass Volume of displaced material that overlies surface of rupture (10) but underlies original ground surface (20) 18 Accumulation Volume of displaced material (13) that lies above original ground surface (20) 19 Flank Undisplaced material adjacent to sides of surface of rupture; compass directions are preferable in describing flanks, but if left and right are used, they refer to flanks as viewed from crown 20 Original ground surface Surface of slope that existed before landslide took place 42 Landslides: Investigation and Mitigation

3.2 Landslide Dimensions ful in remedial work. For instance, for many rota- tional landslides, the surface of rupture can be The IAEG Commission on Landslides (1990) approximated by half an ellipsoid with semiaxes utilized the nomenclature described in Section D, \/2, L/2. As shown in Figure 3-6(a), the 3.1 (including Figure 3-4 and Table 3-3) to pro- volume of an ellipsoid is (Beyer 1987, 162) vide definitions of some dimensions of a typical landslide. The IAEG Commission diagram is VOL=-ica'b' eps 3 reproduced here as Figure 3-5. Once again, each dimension is identified on the diagram by a num- where a, b, and c are semimajor . Thus, the ber, and these numbers are linked to tables giving volume of a "spoon shape" corresponding to one- definitions in several languages. Table 3-4 gives the half an ellipsoid is definitions in English. The quantities Ld, W, Dd and L ,W, D are VOL=--ita•b•c=ira•b'c introduced because, with an assumption about the shape of the landslide, their products to esti- But as shown in Figure 3-6(b), for a landslide mates of the volume of the landslide that are use- a =D, b =W/2, and c =L /2. Therefore, the volume FIGURE 3-5 of ground displaced by a landslide is approximately Landslide dimensions: upper portion, plan VOL =±rca.b.c=±itD .W/2.L/2 of typical landslide 6 6 r r in which dashed line = 17cD W. L is trace of rupture 6 r r surface on original This is the volume of material before the landslide ground surface; lower portion, moves. Movement usually increases the volume of section in which the material being displaced because the displaced hatching indicates material dilates. After the landslide, the volume of undisturbed ground, displaced material can be estimated by 1/6irDdWd Ld stippling shows (WP/WLI 1990, Equation 1). extent of displaced A term borrowed from the indus- material, and broken try, the swell factor, may be used to describe is original ground surface: Numbers increase in volume after as a percen- refer to dimensions tage of the volume before displacement. Church defined in Table 3-4 (1981, Appendix 1) suggested that a swell factor of (IAEG Commission 67 percent "is an average figure obtained from on Landslides 1990). existing data for rock" that has been mechan-

Table 3-4 Definitions of Landslide Dimensions

NUMBER NAME DEFINITION 1 Width of displaced mass, W Maximum breadth of displaced mass perpendicular to length, L 2 Width of surface of rupture, W Maximum width between flanks of landslide perpendicular to length, L 3 Length of displaced mass, Ld Minimum distance from tip to top 4 Length of surface of rupture, L Minimum distance from toe of surface of rupture to crown 5 Depth of displaced mass, Dd Maximum depth of displaced mass measured perpendicular to plane containing Wd and Ld 6 Depth of surface of rupture, D, Maximum depth of surface of rupture below original ground surface measured perpendicular to plane containing W, and L. 7 Total length, L Minimum distance from tip of landslide to crown 8 Length of center line, L 1 Distance from crown to tip of landslide through points on original ground surface equidistant from lateral margins of surface of rupture and displaced material Landslide Types and Processes 43

FIGURE 3-6 (a) Ellipsoid (b) Landslide Estimation of landslide volume assuming a half-ellipsoid shape.

/

ically excavated. His estimates may approximate from the crown despite the frequency of this as- the upper bound for the swell due to landsliding. sumption, originally due to Heim (1932). Material Nicoletti and Sorriso-Valvo (1991) chose an aver- displaced from close to the landslide crown usually age dilation of 33 percent, so 4DWL,. = 3DdWd Ld. comes to rest close to the head of the landslide More precise information is as yet unavailable. Nicoletti and Sorriso-Valvo (1991) proposed that The ground-surface dimensions of the displaced an estimate of the "overall runout" of a landslide be determined by measuring the length of a line con- material, Ld ,Wd, and of the surface of rupture, \X", and the total length, L, of the landslide can be structed along the original ground surface equidis- measured with an electronic distance-measuring tant from the lateral margins of the displaced instrument; a rangefinder may be sufficiently pre- material. However, such may not cise for a one-person reconnaissance. Measure- have immediate physical significance and 'are also ment of the distance L may present problems more difficult and imprecise than measurements of because the toe of the surface of rupture is often L. The length of the landslide measured through not . Its position can sometimes be esti- these central points is called the length of center line, mated from graphical extrapolations of the main L 1. Note that L 1 will increase with the number of scarp supported by measurements of displacements points surveyed on the center line, and the ratio within the displaced mass (Cruden 1986). Al- L 1/L will increase with the curvature of the center though Dd and D1 can also be estimated by these line in plan and section. techniques, site investigations provide more pre- The difference in elevation between the crown cise methods of locating surfaces of rupture under and the tip of the landslide may be used to deter- displaced material (Hutçhinson 1983). mine H, the height of the landslide. Combining The total length of the landslide, dimension L estimates of H and L allows computation of the (5, Figure 3-5), is identical with length L, "the travel angle cx, as shown by Figure 3-7. If the tip is maximum length of the slide upslope," shown in visible from the crown, the travel angle can be mea- Figure 3-3 (Vames 1978); both are the straight- line distances from crown to tip. Readers are cau- tioned that several writers define the length of a landslide in terms of its horizontal extent and fre- quently use the L to define this horizontal distance in tabulations of observations and in cal- culations. This use of L is a source of potential con- fusion and inaccuracy, and readers should make certain that they can identify the dimension being FIGURE 3-7 specified by L in every case. Definition of It should also be emphasized that it is unlikely travel angle (a) that the displaced material at the tip has traveled of a landslide.

Landslides: Investigation and Mitigation

sured directly with a hand clinometer. The H-value and state of activity defined by Vames (1978) and may be conveniently estimated with an altimeter some of his terms defining sequence or repetition when tip and crown are accessible but not visible of movement have been regrouped under three from each other. Hutchinson (1988) compiled data headings: from several different types of debris flows to illus- trate how debris-flow mobility appears to b6 related State of Activity, which describes what is to the travel angle—and to the volume and lithol- known about the timing of movements; ogy of the displaced material (Figure 3-8). Distribution of Activity, which describes The measurements discussed above are ade- broadly where the landslide is moving; and quate during reconnaissance for defining the basic Style of Activity, which indicates the manner dimensions of single-stage landslides whose dis- in which different movements contribute to the placement vectors parallel a common plane. Such landslide. landslides can be conveniently recorded on a land- slide report such as that shown in Figure 3-9. The terms used to define these three characteristics Estimates of landslide volume determined by these of landslide activity are given in the top section of methods are imprecise when diverts Table 3-2 and are highlighted in bold type the first the displacing material from rectilinear paths. time they are used in the following sections. FIGURE 3-8 More elaborate surveys and analyses are then nec- The reader is cautioned that the following dis- Mobility of essary (Nicoletti and Sorriso-Valvo 1991). cussions relate to the terminology proposed by the , chalk UNESCO Working Party (WP/WLI 1990, 1991, debris flows, and 4. LANDSLIDE ACTIVITY 1993a,b) and given in Table 3-2. Other reports and landslides in mine authors may use classifications that apply different wastes related to The broad aspects of landslide activity should be meanings to apparently identical terms. For exam- travel angle (a) and debris volume investigated and described during initial recon- ple, in Chapter 9 of this report, a Unified Landslide (modified from naissance of landslide movements and before more Classification System is introduced that is based on Hutchinson 1988, detailed examinaçion of displaced materials is concepts presented by Figure 12). undertaken. The terms relating to landslide age McCalpin (1984) and Wieczorek (1984). This sys-

60 CHALK KEY H DEBRIS Chalk failures forming a talus 1.6 1EXHIBITING I 0 Chalk failures formIng a flow slIde Flow slide in coal mine waste 1 6 0 Flow slIde in kaolinized talus 76 ApproxImate value of H (m) 21 \ formation More mobile Alpine and Cordilleran + sturzstroms (reported by Hsu,1975) - 45\ Tentative envelope1 for chalk flows >Ce iIopoIpi I- ncreasung 4-. 9Oowreeof Ibergsturzen(Abele,1 975) 40 0.8 sliding I— [3 Zrendlin=orre .Amobiie sturzstroms troms \ D'j 30 I \ -.-.... uJ 82 > 0.4 \ç 20 I- - , 138 085 5 I /' I -- 10 - Mm. volume for granite- IKaolinized I - sturzstroms (Hsu,1975) i —'K.' 10 3 10 4 105 16 10 7 108 10 9

DEBRIS VOLUME () FIGURE 3-9 Proposed standard LANDSLIDE REPORT landslide report form. Inventory Number:

Date of Report: day month year,

Date of Landslide Occurrence: day month year

Landslide Locality:

Reporter's Name:

Affiliation:

Address:

Phone:

Degrees Minutes Seconds

Position: Latitude Longitude

Elevation: crown m a.s.l.

Surface of rupture toe in a.s.l.

tip m a.s.l.

I Geometry: Surface of rupture Displaced Mass L= Ld= L=

wT = Wd

Dr = Dd=

Volume: V= itL,D,Wj6 or V = Swell factor = V= m3 x1O'

Damage: Value

Injuries Deaths 46 Landslides: Investigation and Mitigation

tern is compared with a stability classification pro- moving at present were described by Varnes posed by Crozier (1984). For further information (1978) as suspended. on such alternative systems, the reader should refer Inactive landslides are those that last moved to Tables 9-1, 9-2, and 9-6 and the associated text more than one annual cycle of seasons ago. This in Chapter 9. state can be subdivided. If the causes of movement remain apparent, the landslide is dormant. How- 4.1 State of Activity ever, if the river that has been eroding the toe of the moving slope changes course, the landslide is Figure 3-10 illustrates the several states of activity abandoned (Hutchinson 1973; Hutchinson and by using an idealized toppling failure as an exam- Gostelow 1976). If the toe of the slope has been ple. Active landslides are those that are currently protected against by bank armoring or if moving; they include first-time movements and other artificial remedial measures have stopped reactivations. A landslide that is again active after the movement, the landslide can be described as being inactive may be called reactivated. Slides stabilized. that are reactivated generally move on preexisting Landslides often remain visible in the landscape shear surfaces whose strength parameters approach for thousands of years after they have moved and residual (Skempton 1970) or ultimate (Krahn and then stabilized. Such landslides were called ancient Morgenstern 1979) values. They can be distin- or fossil by Zaruba and Mend (1982, 52), perhaps guished from first-time slides on whose surfaces of because they represent the skeletons of once- rupture initial resistance to shear will generally active movements. When these landslides have approximate peak values (Skempton and Hutch- been covered by other deposits, they are referred inson 1969). Landslides that have moved within to as buried landslides. Landslides that have clearly the last annual cycle of seasons but that are not developed under different geomorphic or climatic conditions, perhaps thousands of years ago, can be called relict. Road construction in southern reactivated relict debris flows that had occurred under periglacial conditions (Skempton and Weeks 1976). Within regions, standard criteria might be FIGURE 3-10 developed to assit in distinguishing suspended Sections through landslides from dormant and relict landslides. topples in different These criteria would describe the recolonization states of activity: by of surfaces exposed by slope move- active—erosion at ments and the dissection of the new topography by toe of slope causes block to topple; . The rate of these changes depends on suspended— both the local and the local vegetation, so local cracking in these criteria must be used with extreme caution. crown of topple; Nevertheless, it is generally true that when the reactivated— main scarp of a landslide supports new vegeta- another block tion, the landslide is usually dormant, and when topples; drainage extends across a landslide without obvi- dormant— displaced mass ous discontinuities, the landslide is commonly begins to regain its relict. However, these generalizations must be con- tree cover and firmed by detailed study of typical slope move- scarps are modified ments under local conditions; Chapter 9 provides by ; a systematic approach for such determinations. stabilized—f luvial Figure 9-7 shows some idealized stages in the evo- stabilizes lution of topographic features on suspended, dor- toe of slope, which mant, and relict landslides. begins to regain its tree cover; and The various states of activity are also defined by relict—uniform an idealized graph of displacement versus time tree cover over slope. (Figure 3-11). For an actual landslide, such a graph Landslide Types and Processes 47

FIGURE 3-1 1 (far left) Displacement of landslide in different states of activity.

FIGURE 3-12 (left) Sections through landslides showing different distributions of activity: advancing, retrogressing, enlarging, diminishing, and can be created by plottiiig differences in the posi- confined. tion of a target on the displacing material with In 1-4, Section 2 time. Such graphs are particularly suited to shows slope after movement on portraying the behavior of slow-moving landslides rupture surface because they presuppose that the target is not dis- indicated by shear placed significantly over the time period during . Stippling which takes place. The of indicates displaced the target can be estimated by the average rate of material. displacement of the target over the time period between measurements. There is some redundancy in using the descrip- tions of activity state with those for rate of move- the surface of rupture may be enlarging, continually ment (see Section 5). Clearly, if the landslide has adding to the volume of displacing material. If the a measurable rate of movement, it is either active surface of rupture of the landslide is enlarging in or reactivated. The state of activity might then be two or more directions, Varnes (1978, 23) sug- used to refer to conditions before the gested the term progressive for the landslide, noting movements of the landslide. If, for instance, reme- that this term had also been used for both advanc- dial measures had been undertaken on a landslide ing and retrogressive landslides. The term is also that is now moving with moderate velocity, the currently used to describe the process by which the landslide might be described as a previously stabi- surface of rupture extends in some landslides (pro- lized, moving, moderate-velocity landslide. Landslides gressive failure). The possibility of confusion seems with no discernible history of previous movement sufficient now to abandon the term progressive in would be described as active. favor of describing the landslide as enlarging. Hutchinson (1988, 9) has drawn attention to con- fined movements that have a scarp but no visible 4.2 Distribution of Activity surface of rupture in the foot of the displaced mass. Varnes (1978) defined a number of terms that can He suggested that displacements in the head of the be used to describe the activity distribution in a displaced mass are taken up by compression and landslide. Figure 3-12 shows idealized sections slight bulging in the foot of the mass. through landslides exhibiting various distributions To complete the possibilities, terms are needed of activity. for landslides in which the volume of material being If the surface of rupture is extending in the direc- displaced grows less with time and for those land- tion of movement, the landslide is advancing, slides in which no trend is obvious. The term dimin- whereas if the surface of rupture is extending in the ishing for an active landslide in which the volume direction opposite the movement of the displaced of material being displaced is decreasing with time material, the landslide is said to be retrogressive. If seems free of undesired implications. A landslide in the surface of rupture is extending at one or both which displaced materials continue to move but lateral margins, the landslide is widening. Move- whose surface of rupture shows no visible changes ment may be limited to the displacing material or can be simply described as moving. Several types of 48 Landslides: Investigation and Mitigation

landslide may exhibit diminishing behavior. Move- tions through landslides exhibiting various styles ment may stop in parts of both rotational slides and of activity. Vames defined complex landslides as topples after substantial displacements because the those with at least two types of movement. How- movements themselves reduce the gravitational ever, it is now suggested that the term complex be on the displaced . Similarly, move- limited to cases in which the various movements ments of rock masses may rapidly dilate cracks in occur in sequence. For instance, the topple the masses, cause decreases in pore pressures described by Giraud et al. (1990) and shown as within these cracks, and hence decrease rates of Figure 3-13(1), in which some of the displaced movement. However, it may be premature to con- mass subsequently slid, is termed a complex rock clude that the displacing material is stabilizing topple—rock slide. Not all the toppled mass slid, but because the volume being displaced is decreasing no significant part of the displaced mass slid with- with time. Hutchinson (1973) pointed out that the out first toppling. Some of the displaced mass may activity of rotational slides caused by erosion at the be still toppling while other parts are sliding. toe of slopes in cohesive soils is often cyclic. The term composite, formerly a synonym for complex, is now proposed to describe landslides in 4.3 Style of Activity which different types of movement occur in differ- ent areas of the displaced mass, sometimes simulta- The style of landslide activity, or the way in which neously. However, the different areas of the different movements contribute to the landslide, FIGURE 3-13 displaced mass show different sequences of move- Sections through can be defined by terms originally established by ment. For example, the structures shown in Figure landslides showing Vames (1978,23). Figure 3-13 shows idealized sec- 3-13(2), first described by Harrison and Falcon different styles of (1934, 1936), were called slide toe topples by activity. (1) Complex: Goodman and Bray (1976), but according to the gneiss (A) and classification proposed in this chapter, they are com- migmatites (I) are posite rock slide—rock topples. The term composite was forming topples introduced by Prior et al. (1968, 76) to describe caused by valley 65, incision; alluvial in which "slipping and sliding. . . occur in materials fill valley intimate association with flowing" and "the mater- bottom; after ial . . . behaves as a liquid and flows rapidly between weathering further confining marginal shears." In the proposed naming weakens toppled convention, such movements are composite earth material, some of slides-earth flows and the convention of treating the displaced mass topographically higher of the two movements as the moves by sliding (modified from first movement and the lower of the two movements Giraud et at. 1990). as the second movement was adopted. Composite: A multiple landslide shows repeated movements have of the same type, often following enlargement of slid on underlying !111111111 the surface of rupture. The newly displaced masses , causing Section Plan are in contact with previously displaced masses toppling failures and often share a surface of rupture with them. In below toe of slide rupture surface a retrogressive, multiple rotational slide, such as that shown in Figure 3-14, two or more blocks have (modified from Cl Harrison and each moved on curved surfaces of rupture tangen- Falcon 1934). tial to common, generally deep surfaces of rupture Successive: (Eisbacher and Clague 1984). later landslide (AB) A successive movement is identical in type is same type as to an earlier movement but in contrast to a multi- landslide CD but ple movement does not share displaced material does not share displaced material or a surface of rupture with it [Figure 3-13(3)]. or rupture surface. According to Skempton and Hutchinson (1969, Single. 297), "successive rotational slips consist of an Landslide Types and Processes 49

( cyv

Comoosite

assembly of individual shallow rotational slips." in its lower limit. These two limits now span 10 FIGURE 3-14 (above) Hutchinson (1967, 116) commented that "irregu-. orders of magnitude. Interpretation of the scale view and lar successive slips which form a mosaic rather was aided by Morgenstern's (1985) analogy to the cross section of typical retrogressive, than a stepped pattern in plan are also found." Mercalli scale of intensity. He pointed multiple rotational out that the effects of a landslide can be sorted into Single landslides consist of a single movement slide (Eisbacher of displaced material, often as an unbroken block six classes corresponding approximately to the and Clague 1984, [Figure 3-13(4)]. For instance, Hutchinson (1988) six fastest movement ranges of Varnes's scale. Figure 10). described single topples in which a single block moved and contrasted these with multiple topples (Figure 3-15). Single landslides differ from the other styles of movement, which require disrup- (a) Single Topple tion of the displaced mass or independent move- ments of portions of the mass.

5. RATE OF MOVEMENT

The previous rate-of-movement scale provided by ubstratu! Varnes (1978, Figure 2.1u) is shown here as Figure 3-16. This scale is unchanged from Varnes's origi- (b) Multiple Topples nal scale (1958) except for the addition of the -41 equivalent SI units, which range from meters per second to millimeters per year. Varnes (1958) did not discuss the divisions of the scale, then given in /;7E units ranging from feet per second to feet per 5 HWM years; the scale probably represented a codification LW M A B LWM of informal practice in the United States at the time. Nem 6ok et al. (1972) suggested a fourfold division of a similar range of . Figure 3-17 presents a modified scale of land- FIGURE 3-15 slide velocity classes. The divisions of the scale Comparison of (a) single topple (Hutchinson 1988) with (b) multiple have been adjusted to increase in multiples of 100 topples [modified from Varnes 1978, Figure 2.1dl ( Freitas and by a slight increase in its upper limit and a decrease Watters 1973)]. 50 /ides: Investigation and Mitigation

FIGURE 3-16 Velocity Description Typical An added seventh class brings these effect classes Varnes landslide (ft/sec) Velocity into correspondence with the divisions of the movement scale velocity scale. (Varnes 1978, The Mercalli scale is based on descriptions of Figure 2.1u). 102 - Extremely Rapid local effects of an earthquake; degrees of damage 101 - ______- 1 Oft/sec = 3 rn/sec can be evaluated by investigating a house or a sec- tion of a . Yet the intensity value can be cor- 100 - Very Rapid related with the total release of the event 10-1 - because both local damage and the area affected are lft/min = 0.3 rn/mm related to the magnitude of the earthquake. The sit- uation is different for landslides. Small, rapid debris

Rapid avalanches are known to have caused total destruc- tion and loss of lives. In contrast, a large slope 1 0 5ft/day = 1.5 rn/day movement of moderate velocity can have much less 1-5— Moderate serious effects because it can be avoided or the - 5ft/mo = 1.5 rn/mo structures affected can be evacuated or rebuilt. It is 10-6 - Slow suggested that a measure of landslide risk should 5ft/yr = 1.5 rn/yr include both the area affected and the velocity; the Very Slow product of these two parameters is approximately 1 08_ proportional to the release of the landslide. - 1ft/5yr = 60 mm/yr Varnes (1984) drew attention to the United 10 9 _ Extremely Slow Nations Disaster Relief Organization terminology in which the specific risk, R,, or the expected degree of loss due to landsliding or any other natural phe- nomenon, can be estimated as the product of the (H) and the vulnerability (V). The hazard is

Velocity Description Velocity Typical the probability of occurrence of the phenomenon Class (mm/sec) Velocity within a given area; the vulnerability is the degree of loss in the given area of elements at risk: popula- 7 Extremely tion, properties, and economic activities. The vul- Rapid nerability ranges from 0 to 1. In this terminology -5x103 5 rn/sec the vulnerability of the landslide might well increase with velocity because it can be expected 6 Very Rapid that extremely rapid landslides would cause greater 5x101 3 rn/mm loss of life and property than slow landslides. A parameter that is difficult to quantify is the Rapid 5 internal distortion of the displaced mass. Struc- tures on a moving mass generally are damaged - 5x10 1.8 rn/hr in proportion to the internal distortion of their 4 Moderate foundations. For example, the Lugnez slope in (Huder 1976) is a 25-km2 area mov- - 5x 1 13 rn/month ing steadily downward at a 15-degree angle at a 3 Slow velocity as high as 0.37 rn/year. The movements have been observed by surveying since 1887. Yet -5x10 5 1.6 rn/year in the six villages on the slope with 300-year-old 2 Very Slow stone houses and churches with bell towers, none of these structures have suffered damage when dis- - 5x10 7 16 mm/year placed because the block is moving without FIGURE 3-17 1 Extremely distortion. Damage will also depend on the type Proposed landslide Slow of landslide, and each type may require separate velocity scale. consideration. Landslide Types and Processes 51

Landslide velocity is a parameter whose destruc- Table 3-5 tive significance requires independent definition. Definition of Probable Destructive Significance of Landslides of Different Velocity Classes Table 3-5 defines the probable destructive signifi- cance of the seven velocity classes on the new LANDSLIDE landslide velocity scale (Figure 3-17). Several case VELOCITY histories in which the effects of landslides on CLASS PROBABLE DESTRucTIvE SIGNIRcANcE and their activities have been well Catastrophe of major violence; buildings destroyed by described and for which the landslide velocities are of displaced material; many deaths; escape unlikely also known are given in Table 3-6, which suggests Some lives lost; velocity too great to permit all persons to a correlation between vulnerability and landslide escape velocity. An important limit appears to lie 5 Escape evacuation possible; structures, possessions, and between very rapid and extremely rapid move- equipment destroyed ment, which approximates the of a person 4 Some temporary and insensitive structures can be running (5 m/sec). Another important boundary temporarily maintained is between the slow and very slow classes (1.6 3 Remedial construction can be undertaken during rn/year), below which some structures on the land- movement; insensitive structures can be maintained with frequent maintenance work if total movement is not large slide are undamaged. Terzaghi (1950, 84) identi- during a particular phase fied as creep those slope movements that were 2 Some permanent structur6 undamaged by movement "proceeding at an imperceptible rate. . . . Typical 1 Imperceptible without instruments; construction possible creep is a continuous movement which proceeds with precautions at an average rate of less than a foot per decade.

Table 3-6 Examples of Landslide Velocity and Damage

LANDSLIDE LANDSLIDE ESTIMATED VELOCITY NAME OR LANDSLIDE CLASS LOCATION REFERENCE VELOCITY DAMAGE 7 Elm Heim (1932) 70m/sec . 115 deaths 7 Goldau Heim (1932) 70 rn/sec 457 deaths 7 Jupille Bishop (1973) 31 rn/sec 11 deaths, houses destroyed 7 Frank McConnell and Brock (1904) 28 rn/sec 70 deaths 7 Vaiont Mueller (1964) 25 rn/sec 1,900 deaths by indirect damage 7 Ikuta Engineering News Record (1971) 18 rn/sec 15 deaths, equipment destroyed 7 St. Jean Vianney Tavenas et al. (1971) 7 rn/sec 14 deaths, structures destroyed 6 Aberfan Bishop (1973) 4.5 rn/sec 144 deaths, some buildings damaged 5 Panama Cross (1924) 1 m/min Equipment trapped, people escaped 4 Handlova Zaruba and Mend (1969) 6 rn/day 150 houses destroyed, complete evacuation 3 Schuders Huder (1976). 10 rn/year Road maintained with difficulty 3 Mountain Palmer (1977) 10 rn/year Road and railway require frequent maintenance, buildings adjusted periodically 2 Lugnez Huder (1976) 0.37 rn/year Six villages on slope undisturbed 2 Little Smoky Thomson and Hayley (1975) 0.25 rn/year protected by slip 2 Klosters Haefeli (1965) 0.02 rn/year maintained, bridge protected by slip joint 2 Ft. Peck Spiliway Wilson (1970) 0.02 rn/year Movements unacceptable, slope flattened 52 Landslides: Investigation and Mitigation

Higher rates of creep movement are uncommon." differences argue against very precise reports of Terzaghi's rate is about 10 mm/sec. The limit of landslide velocity in reconnaissance surveys. perceptible movements on the scale given in Figure 3-17 and Table 3-5 is conservatively lower 6. WATER CONTENT than Terzaghi's. Still lower rates of movement can be detected with appropriate instrumentation Varnes (1978) suggested the following modifica- (Kostak and Cruden 1990). tions to terms first proposed by Radbruch-Hall Vames (1978, 17) pointed out that "creep has (1978) to describe the water content of landslide come to mean different things to different persons, materials by simple observations of the displaced and it seems best to avoid the term or to use it in material: a well-defined manner. As used here, creep is con- sidered to have a meaning similar to that used in Dry: no moisture visible; the mechanics of materials; that is, creep is simply Moist: contains some water but no free water; that continues under constant ." the material may behave as a solid but The term creep should be replaced by the appro- does not flow; priate descriptors from Figure 3-17, either very Wet: contains enough water to behave in part slow or extremely slow, to describe the rate of as a liquid, has water flowing from it, or supports movement of landslides. significant bodies of standing water; and Estimates of landslide velocities can be made by Very wet: contains enough water to flow as a repeated surveys of the positions of displaced liquid under low gradients. objects (Thomson and Hayley 1975; Huder 1976), by reconstruction of the trajectories of portions of These terms may also provide guidance in esti- the displaced mass (Heim 1932; McConnell and mating the water content of the displaced materi- Brock 1904; Ter-Stepanian 1980), by eyewitness als while they were moving. However, soil or rock observations (Tavenas et al. 1971), by instrumen- masses may drain quickly during and after dis- tation (Wilson 1970; Wilson and Mikkelsen 1978), placement, so this guidance may be qualitative and by other means. The Department of rather than quantitative. Individual rock or soil Transportation experimented with the use of time- masses may have water contents that differ con- lapse photography to document the movement of a siderably from the average water content of the FIGURE 3-18 relatively slow-moving but very large landslide. displacing material. For example, Hutchinson Mudslide fabric and The estimates reported were usually the peak veloc- (1988) noted that debris slides (which Hutchinson associated variability ities of substantial portions of the displaced masses; termed mudslides) generally were composed of in water content these estimates are suitable for damage assessments. materials that exhibited a fabric or texture con- (modified from Rates of movement will differ within the displaced sisting of lumps of various sizes in a softened Hutchinson 1988, mass of the landslide with position, time, and the . Samples taken from different portions of Figure 9). period over which the velocity is estimated. Such this fabric had considerably different water con- tents, with lumps having much lower water con-

Location tents than that of the matrix (Figure 3-18). of Typical water-content water-content values for Clay sample 7. MATERIAL - .. Site A Site B (Beltinge) (Sheppey) According to Shroder (1971) and Vames (1978), • \Overall the material contained in a landslide may be Sample 43% 48% described as either rock, a hard or firm mass that was intact and in its natural place before the initi- 'Lump 41% 34% ation of movement, or soil, an of solid ...General , generally of and rocks, that • Matrix 46% 52% either was transported or was formed by the weath- ering of rock in place. Gases or liquids filling the - —True Matrix ?(>46%) ?(>52%) pores of the soil form part of the soil. I ' Soil is divided into earth and debris (see Table 3-1). Earth describes material in which 80 percent Landslide Types and Processes 53 or more of the particles are smaller than 2 mm, the upper limit of -size particles recognized by most geologists (Bates and Jackson 1987). Debris contains a significant proportion of coarse mater- ial; 20 to 80 percent of the particles are larger than 2 mm, and the remainder are less than 2 mm. This division of soils is crude, but it allows the material to be named by a swift and even remote visual inspection. The terms used should describe the displaced material in the landslide before it was displaced. The term rock fall, for instance, implies that the displacing mass was a rock mass at the initiation of the landslide. The displaced mass may be debris after the landslide. If the landslide is complex and the type of movement changes as it progresses, the material should be described at the beginning of each successive movement. For instance, a rock fall that was followed by the flow of the displaced material can be described as a rock fall—debris flow.

8. TYPE OF MOVEMENT

The of a landslide—how movement is distributed through the displaced mass—is one of the principal criteria for classifying landslides. However, of equally great importance is its use as a major criterion for defining the appropriate response to a landslide. For instance, occasional falls from a rock adjacent to a may be contained by a rock fence or similar barrier; in contrast, toppling from the face of the excavation may indicate ad- versely oriented discontinuities in the rock mass that require anchoring or bolting for stabilization. In this section the five kinematically distinct types of landslide movement are described in the sequence fall, topple, slide, spread, and flow (Figure 3-19). Each type of landslide has a number of common modes that are frequently encountered extremely rapid. Except when the displaced mass FIGURE 3-19 in practice and that are described briefly, often has been undercut, falling will be preceded by Types of landslides: with examples of some complex landslides whose small sliding or toppling movements that separate (a) fall, (b) topple, first or initial movements were of that particular the displacing material from the undisturbed mass. (c) slide, ( spread, (e) flow. Broken type. These descriptions show how landslides of Undercutting typically occurs in cohesive soils or that type may evolve. lines indicate original rocks at the toe of a undergoing attack ground surfaces; or in eroding riverbanks. show portions 8.1 FaIl of trajectories of individual particles A fall starts with the detachment of soil or rock 8.1.1 Modes of Falling of displaced mass from a steep slope along a surface on which little [modified from or no shear displacement takes place. The mater- Observations show that the forward of Varnes 1978, Figure ial then descends mainly through the air by falling, masses of soil or rock is often sufficient for free fall 2.1 (Zaruba and bouncing, or . Movement is very rapid to if the slopes below the masses exceed 76 degrees Mend 1969)]. 54 Lands/ides: Investigation and Mitigation

(0.25:1). The falling mass usually strikes a slope 8.2 Topple inclined at less than this angle (Ritchie 1963), A topple [Figure 3-19(b)] is the forward, rotation which causesbouncing. Rebound from the impact will depend on material properties, particularly out of the slope of a mass of soil or rock about a point or axis below the center of of the dis- restitution coefficients, and the angle between the placed mass. Toppling is sometimes driven by grav- slope and the trajectory of the falling mass (Hungr ity exerted by material upslope of the displaced and Evans 1988). The falling mass may also break mass and sometimes by water or ice in cracks in the up on impact. On long slopes with angles at or below 45 mass. Topples may lead to falls or slides of the dis- placed mass, depending on the geometry of the degrees (1:1), particles will have movement paths moving mass, the geometry of the surface of sepa- dominated by rolling. There is a gradual transition ration, and the and extent of the kine- to rolling from bouncing as bounces shorten and matically active discontinuities. Topples range incidence angles decrease. Local steepening of the slope may again project rolling particles into the from extremely slow to extremely rapid, sometimes accelerating throughout the movement. air, restarting the sequence of free fall, bouncing, and rolling (Hungr and Evans 1988). 8.2.1 Modes of Toppling

8.1.2 Complex Falls Flexural toppling was described by Goodman and Bray as Sturzstroms are extremely rapid flows of dry debris created by large falls and slides (Hsu 1975). These occurring in rocks with one preferred disconti- flows may reach velocities over 50 m/sec. Sturzs- nuity system, oriented to present a rock slope troms have also been called rock-fall avalanches with semi-continuous cantilever beams. (Varnes 1958) and rock avalanches (Evans et al. Continuous columns break in flexure as they 1989; Nicoletti and Sorriso-Valvo 1991). Two bend forward.... Sliding, undermining or ero- examples of historic sturzstroms in Switzerland, sion of the toe (of the displaced mass) lets the the Rossberg landslide of 1806 and the Elm land- failure begin and it retrogresses backwards with slide of 1881, are discussed in Chapter 1. Hsu deep, wide tension cracks. The lower portion (1975) suggested that 5 million m3 is the lower of the slope is covered with disoriented and dis- limit of the volume of significant sturzstroms, but ordered blocks. . . . The outward movement of Hutchinson (1988) demonstrated that falls in each cantilever produces interlayer sliding high-, weak European chalk rocks with (flexural slip) and. . . back-facing scarps (obse- volumes two orders of magnitude smaller have the quent scarps). . . . It is hard to say where the same exceptional mobility because of collapse of base of the disturbance lies for the change is the pores on impact and consequent high pore- gradual. . . . Flexural toppling occurs most water. pressures. Some of Hutchinson's data are notably in , phyllites and . (Good- reproduced in Figure 3-19. man and Bray 1976, 203) The motion of sturzstroms probably depends on A flexural topple in the proposed classification is a turbulent grain flow with dispersive stresses arising retrogressive, complex rock topple—rock fall. Typical from transfer between colliding grains. examples are shown in Figures 3-20(a) and 15-16. Such a mechanism does not require the presence In contrast, block toppling occurs of a liquid or gaseous pore fluid and can therefore explain lunar and Martian sturzstroms. Van Gassen where the individual columns are divided by and Cruden (1989) showed that the motion of the widely-spaced joints. The toe of the slope with complex, extremely rapid, dry rock fall—debris flow short columns, receives load from overturning, that occurred near the town of Frank, Alberta, longer columns above. This thrusts the toe Canada, in 1903 (see Figure 3-1) could be explained columns forward, permitting further toppling. reasonably well by momentum exchange between The base of the disturbed mass is better defined the moving particles and measured coefficients of than in the case of flexural toppling; it consists . of a stairway generally rising from one layer to Landslide Types and Processes 55

the next. The steps of this stairway are formed by cross-joints. . . . New rock breakage occurs much less markedly than in flexural topples.. . . Thick-bedded sedimentary rocks such as limestones and , as well as columnar-jointed volcanics exhibit block- toppling. (Goodman and Bray 1976, 203)

Typical examples of block toppling are shown in Figure 15-16. Chevron topples are block topples in which the dips of the toppled beds are constant and the change of dip is concentrated at the surface of rup- ture (Cruden et al. 1993). This mode was named from its resemblance to chevron folds (Ramsay 1967, 436). Chevron topples occur on steeper slopes than other block topples. The surface of rupture is often a sliding surface [Figure 3-20(b)] forming a complex rock topple—rock slide. Block-flexure toppling is characterized by

pseudo-continuous flexure of long columns through accumulated along numerous cross joints. Sliding is distributed along several joint surfaces in the toe [of the displaced mass] while sliding and overturning occur in close association through the rest of the mass. (Goodman and Bray 1976, 204)

Sliding occurs because accumulated overturning steepens the cross joints. There are fewer edge-to- face contacts than in block toppling but still enough to form "a loosened, highly open . . . dis- turbed zone [displaced mass].... Interhedded sand- stone and , interbedded chert and shale and thin-bedded exhibit block flexure top- pling" (Goodman and Bray 1976, 204). Typical block-flexure topple examples are shown in Figures 3-20(c) and 15-16. FIGURE 3-20 Three modes of toppling. (a) Flexural: cracks indicate tension-crack topple; fallen blocks below topple show movement is complex rock topple—rock 8.2.2 Complex and Composite Topples fall. (b) Chevron: multiple block topple; hinge surface of chevron may develop into surface of rupture of slide forming complex multiple rock A complex rock topple—rock slide is shown in Figure topple—rock slide. (c) Block-flexure. 3-130). This cross section of the La Clapière land- slide was described by Giraud et al. as follows: result of deformation of the massif. (Giraud Several distinct movements may be identified et al. 1990, 250) as the phenomenon progresses, along with a modification of water flows within the rock Goodman and Bray (1976) identified four com- mass, due to considerable changes in perme- posite landslide modes in which toppling was ability over time and probably in as a caused by earlier sliding. These landslide condi- 56 Landslides: Investigation and Mitigation

dons are discussed in detail in Chapter 15 and are beyond the toe of the surface of rupture covering illustrated in Figure 15-17. A slide head topple the original ground surface of the slope, which occurs as blocks from the crown of the slide topple then becomes a surface of separation. onto the head of the displaced mass. According to the naming convention, such a landslide is a com- 8.3.1 Modes of Sliding posite rock slide—retrogressive rock topple. Rotational sliding of earth or debris above a Varnes (1978) emphasized the distinction between steeply dipping mass can cause rotational and translational slides as significant for slide base toppling as the sliding induces shear forces stability analyses and control methods. That dis- in the top of the rock mass (Goodman and Bray tinction is retained in this discussion. Figure 3-22 1976). The resulting landslide is, according to shows two rotational slides and three translational the proposed naming convention, a composite earth slides. Translational slides frequently into slide—advancing rock topple. flows or spreads. Toppling below the toe of the surface of rupture Rotational slides (Figure 3-23) move along a sur- of a rock slide may be caused by load transmitted face of rupture that is curved and concave. If the from the slide. Such a failure is called a slide toe top- surface of rupture is circular or cycloidal in profile, ple (Goodman and Bray 1976). According to the kinematics dictates that the displaced mass may proposed naming convention, it is a composite move along the surface with little internal defor- rock slide—rock topple. mation. The head of the displaced material may The formation of extension cracks in the crown move almost vertically downward, whereas the of a landslide may create blocks capable of top- upper surface of the displaced material tilts back- pling, or a tension crack topple (Goodman and Bray ward toward the scarp. If the slide extends for a 1976). According to the proposed naming con- considerable distance along the slope perpendicu- vention, this is a retrogressive multiple topple, per- lar to the direction of motion, the surface of rup- haps forming part of a composite fall or slide. Such ture may be roughly cylindrical. The axis of the failures may also occur in cohesive soils being cylindrical surface is parallel to the axis about undercut along streambanks (Figure 3-21). which the slide rotates. Rotational slides in soils generally exhibit a ratio of depth of the surface of 8.3 Slide rupture to length of the surface of rupture, D /L (see Table 3-4 and Figure 3-5 for definitions A slide is a downslope movement of a soil or rock of these dimensions), between 0.15 and 0.33 mass occurring dominantly on surfaces of rupture (Skempton and Hutchinson 1969). or on relatively thin zones of intense shear strain. Because rotational slides occur most frequently Movement does not initially occur simultaneously in homogeneous materials, their incidence in fills over the whole of what eventually becomes the has been higher than that of other types of move- surface of rupture; the volume of displacing mate- ment. Natural materials are seldom uniform, how- rial enlarges from an area of local failure. Often the FIGURE 3-21 ever, and slope movements in these materials Debris topple first signs of ground movement are cracks in the commonly follow inhomogeneities and disconti- (Varnesi 978, original ground surface along which the main scarp nuities (Figure 3-24). Cuts may cause movements Figure 2.1e). of the slide will form. The displaced mass may slide that cannot be analyzed by methods used for rota- tional slides, and other more appropriate methods have been developed. Engineers have concen- trated their studies on rotational slides. The scarp below the crown of a rotational slide may be almost vertical and unsupported. Further movements may cause retrogression of the slide into the crown. Occasionally, the lateral margins of the surface of rupture may be sufficiently high and steep to cause'the flanks to move down and into the depletion zone of the slide. Water finding its way into the head of a rotational slide may con-

Landslide Types and Processes 57

FIGURE 3-22 Examples of rotational and translational slides: (a) rotational rock slide; (b) rotational earth slide; (c) translational rock slide (upper portion is rock block slide); (a) debris slide; (e) translational earth block slide[Varnes 1978, Figures 2.1g, 2.1i, 2.1j2, 2.1k, 2.11 (Hansen 1965)].

tribute to a sag pond in the backward-tilted, dis- placedmass. This disruption of drainage may keep the displaced material wet and perpetuate the •. slope movements until a slope of sufficiently low r . gradient is formed. In translational slides (Figures 3-22, 3-25, and \'. S-S .,• S 3-26) the mass displaces along a planar or undu- lating surface of rupture, sliding out over the orig- L I : inal ground surface. Translational slides generally k.. S.. are relatively shallower than rotational slides. Therefore, ratios of D,JL,. for translational slides in ::-''- ,.. S.. soils are typically less than 0.1 (Skempton and 5.5 Hutchinson 1969). The surfaces of rupture of S.-. •55 - translational slides are often broadly - (Hutchinson - shaped in cross section 1988). - '- - k '- . 4••.S Z... . Whereas the rotation of a rotational slide tends to restore the displaced mass to equilibrium, transla- tion may continue unchecked if the surface of FIGURE 3-23 separation is sufficiently inclined. Cut through rotational slide of fine-grained, thin-bedded deposits, As translational sliding continues, the displaced Columbia River valley; beds above surface of rupture have been rotated by mass may break up, particularly if its velocity or slide to dip in slope (Varnes 1978, Figure 2.7).

58 Lands/ides: Investigation and Mitigation

FIGURE 3-24 I.) SLOPE FAILURE IN HOMOGENEOUS MATERIAL. Ib) SLOPE FAILURE IN NONHOMOGENEOUS MATERIAL. Rotational slides CIRCULAR ARC. Ill SLIDE WHOLLY ON SLOPE AND SURFACE OF RUPTURE FOLLOWS DIPPING WEAK (2) SURFACE OF RUPTURE INTERSECTS TOE OF . (Varnes 1978, SLOPE. Figure 2.5).

r2 \ oft T r cl oy

shall

(c) BASE FAILURE IN HOMOGENEOUS CLAY. SLIP IdI BASE FAILURE IN NONHOMOGENEOUS MATERIAL. CIRCLE TANGENT TO FIRM BASE, CENTER ON SURFACE OF RUPTURE FOLLOWS BED OF VERY VERTICAL BISECTOR OF SLOPE. SOFT CLAY.

roben irm loy

rrnedId

I.) SLIDE BENEATH SIDE HILL . Sol (II FAILURE WITHIN A SIDEHILL FILL.

CU'\OriinaI ground line

Sand- stone Fill Fill Coal Clay

"Shole

FIGURE 3-25 (g) FAILURE OF . COUNTER. (h) SLIDE IN FILL INVOLVING UNDERTHRUSTING OF (be/ow) WEIGHT ON LEFT SIDE PREVENTS SLIDE. FIRM SURFACE MATERIAL DOWN SLOPE. Translational slide Fill of Firm Fill on inclined counterweig !~F. Il a r metasiltstone strata along -40, Soft zone- Cocke County, (Varnes Stable 1978, Figure 2.11). FEZ Firm

water content increases. The disrupted mass may then flow, becoming a debris flow rather than a slide. Translational sliding often follows disconti- nuities such as faults, joints, or bedding surfaces or the contact between rock and residual or trans- ported soils. Translational slides on single discontinuities in tuck masses have beeti called block slides (Paiiet 1969) or planar slides (I- and Bray 1981). As e - Hutchinson (1988) pointed out, there is a transi- lion from rock slides of moderate displacement that remain as blocks on the surface of rupture to slides

. -'.. . 41 on steeper and longer surfaces that break up into debris or transform into sturzstroms. Where the sur- Landslide Types and Processes 59 face of rupture follows a discontinuity that is paral- lel to the slope, the toe of the displaced mass may form a wedge that overrides or ploughs into undis- placed material causing folding beyond the toe of the surface of rupture (Walton and Atkinson 1978). Composite rock slide—rock ropples [Figure 313(2)] or buckles and conned slides may result. The surface of rupture may be formed by two discontinuities that cause the contained rock mass to displace down the line of intersection of the dis- continuities, forming a wedge slide [Figure 3-27(a) and Chapter 15, Figures 15-8 through 15-141. Similarly shaped displaced masses may be bounded by one discontinuity that forms the main scarp of the slide and another that forms the surface of rup- ture. The mode of movement depends on the ori- entations of the free surfaces relative to the discontinuitics in the rock masses (Hocking 1976; Cruden 1978, 1984). Stepped rupture surfaces may result if two or more sets of discontinuities, such as bedding surfaces and some joint sets, penetrate the rock masses. As shown in Figure 3-27(b), one set FIGURE 3-26 (above) of surfaces forms the risers of the steps and the Shallow translational other forms the treads, creating a stepped slide slide that developed (Kovari and Fritz 1984). on shaly rock slope Compound slides are intermediate between rota- in Puente Hills of tional and translational slides and their D IL ratios southern California; reflect this position (Skempton and Hutchinson slide has low D/L Surfaces of rupture have steep main scarps ratio; note wrinkles 1969). on surface [Varnes that may flatten with depth [Figure 3-22(e)]. The 1978, Figure 2.33; toes of the surfaces of rupture may dip upsiope. (Shelton 1966)]. Displacement along complexly curved surfaces of (X)IYRlGHT JOI INS. ShELTON rupture usually requires internal deformation and shear along surfaces within the displaced material FIGURE 3-27 and results in the formation of intermediate scarps. (left) Abrupt decreases in downslope dips of surfaces of Wedge and rupture may be marked by uphill-facing scarps in stepped displaced masses and the subsidence of blocks of translational slides. displaced material to form depressed areas, grabens [Figure 3-22(e)]. A compound slide often indicates the presence of a weak layer or the boundary be- tween weathered and unweathered material. Such erences to a variety of specialized names. Two of zones control the location of the surface of rupture these names, mudslide and flowslide, are believed to (Hutchinson 1988). In single compound slides, the be imprecise and ambiguous, and therefore their width of the grahen may be proportional to the use is not recommended. depth to the surface of rupture (Cruden et al. 1991). According to Hutchinson, mudslides are

slow-moving, commonly lobate or elongate 8.3.2 Complex and Composite Slides masses of accumulated debris in a softened Complex and composite slide movements are clayey matrix which advance chiefly by sliding common and the literature contains numerous ref- on discrete, bounding shear surfaces. - . - In Wt Landslides: Investigation and Mitigation

long profile, mudslides are generally bilinear . Landslides occurring in loosely dumped an- with a steeper . . . slope down which debris is thropogenic materials, both stockpiles and waste fed (by falls, shallow slides and mudslides) to a dumps, have also been termed flowslides. These more gently-inclined slope. . . . Mudslides are loose, cohesionless materials contract on shearing especially well-developed on slopes containing and so may generate high pore-water pressures after stiff, fissured clays, doubtless because of the ease some sliding (Eckersley 1990). Similar landslides with which such materials break down to pro- may also occur in rapidly deposited natural and vide a good debris supply. (Hutchinson 1988, fine (Hutchinson 1988, 14). Since these 12-13) movements involve both sliding and then flowage, they may be better described as complex slide flows. Evidently these movements begin in either Because these separate and distinguishable phe- weak rock or earth and retrogress by falls and slides nomena are comparatively distinct types of land- while advancing by sliding. Hutchinson and Bhan- slides that may be more accurately described by dan (1971) suggested that the displaced material, standard descriptors, the use of the term flowslide fed from above onto the mudslide, acted as an un- for all these types of movements is redundant, con- drained load. Clearly mudslides are composite or fusing, and potentially ambiguous. perhaps complex both in style of activity and in the In contrast, one form of compound sliding fail- breakdown of displaced material into earth or ure appears to warrant a special term. Sags (or sack- debris. The displaced material is generally moist, ungen) are deformations of the crests and steep though locally it may be wet. A mudslide is there- slopes of mountain that form scarps and fore often a retrogressive, composite rock slide— grabens and result in some ridges with double advancing, slow, moist earth slide. Other mudslide crests and small summit . Material can be dis- modes may include single earth slides (Brunsden placed tens of meters at individual scarps. The 1984). The current use of mudslide for several dif- state of activity, however, is generally dormant and ferent landslide modes suggests that more precise may be relict. The term sag may be useful to indi- terminology should be used where possible. cate uncertainty about the type of movement vis- The term flowslide has been used to describe sud- ible on a mountain . den collapses of material that then move consid- Movement is often confined, and small bulges erable distances very rapidly to extremely rapidly. in local slopes are the only evidence of the toes of As Hutchinson (1988) and Eckersley (1990) the displaced material. Detailed subsurface inves- pointed out, at least three phenomena can cause tigations of these features are rare, and classifica- this behavior: (a) impact collapse, (b) dynamic tion should await this more detailed exploration. liquefaction, and (c) static liquefaction. Impact- As Hutchinson (1988,8) demonstrated, the geom- collapse flowslides occur when highly porous, etry of the scarps (which often face uphill) may be often-saturated weak rocks fall from cliffs, resulting used to suggest types of movement, which may in destruction of the of the material and include slides, spreads, and topples. The modes of the generation of excess fluid pressures within the sagging depend on the lithobogy of the displaced flowing displaced mass. Clearly these are complex material and the orientation and strength of the falls in which the second mode of movement is a discontinuities in the displacing rock mass. Vames debris flow; if the displaced material is dry debris, et at. (1989, 1) distinguished the movement may be a , previously defined in Section 8.1.2. This mode of movement "Massive, strong (although jointed) rocks lying can be recognized by both the materials involved on weak rocks," and the topography of the flow. "Ridges composed generally of metamorphosed If the structure of the material is destroyed by rocks with pronounced foliation, schistosity or shocks such as , saturated material may ," and liquefy and then flow, sometimes carrying masses of "Ridges composed of hard, but fractured, crys- overlying drier material with it. Such a movement talline igneous rocks." is a flow or liquefaction spread, which is further defined in Section 8.4.1. Such movements are Sags of the first type are usually spreads characteristic of bess, a lightly cemented aeolian (Radbruch-Hall 1978; Radbruch-Hall et al. 1976), Landslide Types and Processes which are discussed in Section 8.4. Sags in foliated FIGURE 3-28 metamorphic rocks are often topples, and thus are rrd Plan of Ames slide 1po,,d near Telluride, discussed in Section 8.2, although bedrock flow ZONE A Mon.,n.,,t dtinfly by ,, Colorado. This may also occur (see Section 8.5). Sags in crys- wole don,ping along dip surfaces A" - enlarging complex A. A', A' talline igneous rocks (Varnes et al. 1989, 22) were PrIncIpot dotnp eriitt earth slide—earth 8,8' — modeled by a solution for "gravity- Narrow glomp oni, with flow occurred in rpendicular to / ::of mwn units induced deformation of a slope yielding under the length overlying Mancos of —in slide shale. Crown of Coulomb criterion." Sags may thus be slides, C ' remaining after downward movement of slide retrogressed by spreads, or flows, depending on the extent and unit D from ,raE. P multiple rotational flow within the deforming distribution of plastic slides after main rock mass. - body of displaced Sags are often associated with glacial features. material moved. The absence of snow and ice covers, ZONEB - — - Surface of rupture Zone of earth flow; — - movement ohinfly by — - -' and the resulting loss of the and high fiowo. also widened on left lateral margin pore-water pressures these induced, may account —— for the present inactivity of many sags. Varnes et [Varnes 1978, Figure 2.10 (modified from al. (1990) described an active sag in the mountains Varnes 1949)]. of Colorado. Earthquakes, however, can also pro- Toe of slide ama:ogal duce uphill-facing scarps along reactivated normal for altered by railroad reconstructiOn work. , •, I faults. The surface features of sags require careful / investigation before any conclusions can be drawn tOOm about the cause and timing of slope movement. Such investigations may be sufficient to allow the identification of sags as other types of landslides. In many landslides, the displaced material, ini- tially broken by slide movements, subsequently begins to flow (Figure 3-28). This behavior is espe- It is characteristic . . . that a gentle clay slope cially common when fine-grained or weak materi- which may have been stable for decades or cen- als are involved. These landslides have been turies, moves out suddenly along a broad front. At the same time the terrain in front... heaves termed slump-earth flows. Slump has been used as a synonym for a rotational slide, but it is also used to for a considerable distance from the toe. On investigation, it has invariably been found that describe any movement in a fill. It is therefore rec- the spreading occurred at a considerable dis- ommended that this mode of movement be termed tance beneath the toe along the boundary complex earth slide—earth flow and that the use of a between the clay and an underlying water- be discontinued. the term slump or seam of sand or silt. (Ter- In permafrost regions, distinctive retrogressive, zaghi and Peck 1948, 366) complex earth slide—earth flows, known as thaw- slumps (Hutchinson 1988, 21) and bimodal flows Recognition of the phenomenon is considerably (McRoberts and Morgenstem 1974), develop on older. One of the three types of landslides distin- steep earth slopes when icy permafrost thaws and guished by Dana (1877, 74) occurs "when a layer forms flows of very wet from a steep main of clay or wet sand becomes wet and softened by scarp. These special landslide conditions are dis- percolating water and then is pressed Out laterally cussed in more detail in Chapter 25. by the weight of the superincumbent layers." An early use of spread to describe this phenomenon is 8.4 Spread by Barlow:

The term spread was introduced to geotechnical In a landslip [British term for some types of engineering by Terzaghi and Peck (1948) to landslide], the spreading of some underlying bed describe sudden movements on water-bearing which has become plastic through the percola- seams of sand or silt overlain by hdmogeneous tion of water or for some other cause drags apart clays or loaded by fills: the more solid, intractable beds above and pro- 62 Landslides: Investigation and Mitigation

duces fissures and fractures transverse to the may also fill with broken, displaced material direction of movement. (Barlow 1888, 786) [Figure 3-29(a)]. Typical rates of movement are extremely slow. Spread is defined here as an extension of a cohe- Such movements may extend many kilometers sive soil or rock mass combined with a general sub- back from the edges of and . sidence of the fractured mass of cohesive material The Needles District of Canyonlands National into softer underlying material. The surface of rup- Park, Utah, is an example of a block spread (McGill ture is not a surface of intense shear. Spreads may and Stromquist 1979; Baars 1989). Grabens up to result from liquefaction or flow (and extrusion) of 600 m wide and 100 m deep stretch 20 km along the softer material. Vames (1978) distinguished the east side of Cataract Canyon on the Colorado spreads typical of rock, which extended without River (Figure 3-30). The grabens extend up to 11. forming an identifiable surface of rupture from km back from the river. A 450-rn-thick sequence movements in cohesive soils overlying liquefied of Paleozoic sedimentary rocks has been spread materials or materials flowing plastically (Figure down a regional slope with a 4-degree dip by the 3-29). The cohesive materials may also subside, flow of an underlying evaporite that is exposed in translate, rotate, disintegrate, or liquefy and flow. valley anticlines in the Colorado River and its trib- Clearly these movements are complex, but they are utaries (Potter and McGill 1978; Baars 1989). This sufficiently common in certain materials and geo- approximately 60 km3 of displaced material con- logical situations that the concept of a spread is stitutes one of North America's largest landslides. worth recognizing as a separate type of movement. Liquefaction spreads form in sensitive clays and silts that have lost strength with disturbances that 8.4.1 Modes of Spreading damaged their structure [Figures 3-29(c) and 3-3 1]. These types of landslides are discussed fur- In block spreads, a thick layer of rock overlies softer ther in Chapter 24. Movement is translational and materials; the strong upper layer may and often retrogressive, starting at a bank or a separate into strips. The soft underlying material is shoreline and extending away from it. However, if squeezed into the cracks between the strips, which the underlying flowing layer is thick, blocks may

(a) 1 50. 100 50

FIGURE 3-29 0 500 Rock and earth spreads: (a), (b) rock spreads that have (b) experienced lateral extension without well-defined basal shear surface or zone of plastic flow [Varnes 1978, Figure 2.1m2 (Zaruba and (C) Mend 1969); Figure

2.1m3 (Ostaficzuk Fi,m 1973)]; earth (c) Solt clay with wate,-be spread resulting silt and sand layers from liquefaction Fi,m claye or plastic flow of subjacent material (Varnes 1978, Figure 2.1o). Landslide Types and Processes 63 sink into it, forming grahens, and upward flow can take place at the toe of the displaced mass. Move- ment can begin suddenly and reach very rapid velocities:

Spreads are the most common ground failure during earthquakes. .. . [They] occur in gentler (commonly between 0.5 per cent [0.3 degrees] and 5 percent [3 degrees]) with lateral movement of a few meters or so. . . . [S]preads involve fracturing and extension of coherent material owing to liquefaction or plastic flow of subjacent material. . . . [S]preads are primarily translational although some associated rota- tion and subsidence commonly occurs. (Andnis and Youd 1987, 16)

Van Horn (1975) described two movements of more than 8 km2 in area on very gentle slopes in -lying beds of silty clay, clayey silt, and very fine FIGURE 3-30 sand deposited in prehistoric Lake Bonneville, Geological cross section showing formation of The Grabens in Needles Utah. The displaced material forms ridges parallel District of Canyonlands National Park, Utah. Colorado River has carved to the main scarp of the landslide; distinctive Cataract Canyon to within a few meters of top of Paradox Salt beds (IPps), internal structures include gentle folds, shears, and undercutting inclined layers of overlying Honaker Trail (IPht), Elephant Canyon (Pec), and Cedar Mesa (Pcm) formations. These formations have intrusions of liquefied . broken up and are moving toward canyon by flowage within salt. Colorado River follows crest of anticline, a salt-intruded located above 8.4.2 Complex Spreads a deep-seated zone (Baars 1989). Major deformations in rock strata were found along many valleys in north-central England dur- -. - ing the construction of in the late 19th cen- tury. These deformations occurred where a nearly .1.. horizontal, rigid-joinied cap tuck uveilaid a iltick layer of stiff-fissured clay or clay shale that in turn overlaid a more competent stratum. A bending, or cambering, of the rigid strata caused blocks of this stratum to dip toward the valley. This bending of the upper stratum was accompanied by severe deformation and bulging of the softer lower strata in the valley floor. Hutchinson (1991) defined characteristic fea- tures of cambers and valley bulges as follows:

Marked thinning of the clay substratum as a result of the transfer of clay into the valley bulge; Intense folding and distortion in the valley bulge FIGURE 3-31 Earth spread—earth flow near Greensboro, Florida. Material is flat-lying, itself as a result of the meeting of the clay masses partly indurated clayey sand of Hawthorn Formation. Length of slide is moving in from beneath each valley side; 275 m from scarp to edge of trees in foreground. Vertical distance is about Sympathetic flexuring of the superincumbent 15 m from top to base of scarp and about 20 m from top of scarp to toe. capping rocks, producing a valleyward camber, Landslide occurred in April 1948 after a year of unusually heavy rainfall, a valley marginal syncline, and an upturn including 40 cm in the 30 days preceding landslide [Varnes 1978, Figure against the flanks of the bulge; and 2.19 (modified from Jordan 1949)]. 64 Landslides: Investigation and Mitigation

Extension and valleyward toppling of the cap- exaggeration. Figure 3-32(b) is based on a diagram ping rocks in the camber, resulting in opening of by Hutchinson (1991) that shows the same general near-vertical joints to form wide-open fissures, section without vertical exaggeration and empha- termed gulls, in valleyward dips of the camber sizes that the displaced materials are found on blocks and in the development of dip-and-fault slopes of less than 5 degrees. According to the pro- structures between camber blocks as a conse- posed naming convention, a camber may be de- quence of their toppling. scribed as a relict, complex rock spread—rock topple. Ward (1948) described as a landslide another The rotation of the dip of the rock blocks pro- complex spread in Britain in which stiff-fissured duces the slightly arched or convex form popularly clays overlaid fine sands but qualified his descrip- called a camber. Rotation is made possible by the tion as follows: extension of "the cap-rock towards the valley pro- ducing widened joints (called gulls) often infilled So much movement of various types had by till" (Hutchinson 1988, 19). The cap rock has occurred that it was difficult to trace the move- spread. The underlying clay exhibits ment of the strata from the upper cliff until it arrived in the form of mud on the some a brecciated structure, probably frost- induced, 180 feet below.... The underlying fine sand is in its upper parts, marked thinning as the in a saturated, quick condition under the valley is approached and intense generally- blocks when they become detached and they FIGURE 3-32 monoclinal folding in . . . the present valley probably flounder forwards and tilt backwards. Cambering and valley bulging at bottom. . . . The dramatic internal structures (Ward 1948, 36) Empingham, appear to be the result principally of valley- England: ward squeezing and extrusion made possible This description suggests that the clay was being detailed cross by the weakening of the clay stratum by mul- spread by the flow of the sand and thus the move- section with 4x tiple freezing and thawing.. . . These cambers ment was a type of complex earth spread—debris flow. vertical exaggeration and valley bulges are believed to be relict (modified from periglacial features. (Hutchinson 1988, 19) 8.5 Flow Horswill and Horton 1976); and Cambering and valley bulging affected slopes at A flow is a spatially continuous movement in generalized Empingham, England, that were excavated during which surfaces of shear are short-lived, closely cross section drawn without vertical the construction of a (Horswill and Horton spaced, and usually not preserved. The distribution exaggeration 1976). Figure 3-32(a) reproduces a portion of Fig- of velocities in the displacing mass resembles that (modified from ure 5 of Horswill and Horton (1976), which shows in a viscous liquid. The lower boundary of the dis- Hutchinson 1991). the details of the structures with a fourfold vertical placed mass may be a surface along which appre-

Normal Sub-horizontal (a) Camber slope.

Cap rock Dip and

by eroslon)

Cly

- - - - - fleOfdeoobemt!

(b)

rrerresOo J...... _Ptelitu.e PmlIizO.0 roiioc.o—.j 120 120 o 00 togo H,od 80 HeIdI 40 Mzrltonr Rock Bad 4020 20 Middle Lien Silt, and C1e1, 0 -500 -00 -300 -200 -100 0-100 -200 -300 -400 -500 -600 -700 -800 -900 Darn Cheiroge (n.) Pipolir, Choir09.)...) Landslide Types and Processes 65 ciable differential movement has taken place or a FIGURE 3-34 Channelized distributed shear (Figure 3-33). Thus thick zone of debris flows: there is a gradation from slides to flows depending debris flow, on water content, mobility, and evolution of the debris , movement. Debris slides may become extremely and (c) block stream rapid debris flows or debris avalanches as the dis- (Varnes 1978, placed material loses cohesion, gains water, or Figures 2.1q1, encounters steeper slopes (Figure 3-34). 2.1q3, 2.1q5). Varnes (1978, 19-20) used the terms earth flow and slow earth flow [Figure 3-33(a)] to describe "the somewhat drier and slower earth flows in plastic earth. . . common... wherever there is. . . clay or weathered clay-bearing rocks, moderate slopes, and adequate moisture." Weathered bedrock. Keefer and Johnson (1983) included detailed Soil etc studies of the movement of earth flows in the San Bedrock Francisco area (Figure 3-3 5). They concluded (Keefer and Johnson 1983, 52): "Although some internal deformation occurs within earth flows,

(C)

most movement takes place on or immediately adjacent to their boundaries." Their use of earth Terraced Letds

Lake flow thus covers landslide modes from slow earth flow through slow, composite earth slide—earth flow to slow earth slide. When extensive, striated, or slickensided lateral margins or surfaces of rupture are visible, the landslide might well be called an earth slide; when the displaced mass is strongly FIGURE 3-33 deformed internally, the landslide is probably an Examples of flows: -\ earth flow. If the same landslide shows both modes slow earth flow & Dry sand \ ' of deformation, it is clearly a composite earth [Varnes 1978, Figure slide—earth flow. 2.1r3 (Zaruba and Fare cdl Mend 1969)], While defining landslide processes in perma- Sand bess flow, and frost regions, McRoberts and Morgenstern (1974) dry sand flow used the term skin flow to describe a rapid to very (Varnes 1978, rapid slope movement in which a thin layer, or Figures 2.1r5 skin, of thawed soil and vegetation flows or slides and 2.1r4). Wl Landslides: Investigation and Mitigation

FIGURE 3-35 or may extend as sheets for some distance across a Earth flow slope [Figure 3-33(h) and 3.37]. developing from Channelzzed flows follow existing channels (Fig- initial rotational ures 3-34 and 3-38). As earth slide near shown in Figure 3-39, Berkeley, California debris flows are often of high density, with over 80 (Varnes 1978, percent by weight, and may exceed the den- Figure 2.22). sity of wet (Hutchinson 1988). They can therefore move that are meters in diame- ter. The mode of flow shown in Figure 3-40 often occurs during torrential rIlnff following excep- tional rainfalls. Soils on steep slopes unprotected by vegetation whose natural cover may have been destroyed by are prone to debris flows. Debris may be added to small surface by erosion or of their banks, increasing the power of over the permafrost table, whereas Hutchinson the flows. Coarser material may form natural lev- (1988, 12) used the term active-layerslide. Seasonal ees, leaving the fines in suspension to move down thaw layers, or active layers, up to a meter or so in the channel. Flows can extend many kilometers thickness may contain water originally drawn to before they drop their suspended loads upon enter- the freezing front where it formed segregated ice. ing lower-gradient channels. The movement may Melting of this ice may generate artesian pore- be in pulses, presumably caused by periodic mobi- water pressures that greatly reduce the resistance lization of material or by the formation and burst- of the to movement. These landslide ing of dams of debris in the channel. conditions are discussed in more detail in Chapter Pierson and Costa (1987) observed that the 25. Similar shallow failure may also occur in bess term debris torrent was misleading and gave two materials that become saturated or are subjected to reasons: earthquake shaking [Figure 3-33(b)]. Open-slope debris flows form their own First, mountain torrent or debris torrent is used down a valley side onto the gentler slopes at the in European and Japanese literature to mean a foot. Deposition of there may outline a more very steep channel, not the material that flows sinuous channel. The common, small dry flows of in it. . . . Second, the term was coined to dif- may be channelized (Figure 3-3 6) ferentiate between coarse debris flows occur- ring in channels and flows occurring on open slopes . . . , a criterion that has no rheologic or other process-specific basis. suggest that the usage of the term, debris torrent, be discontin- ued and the more general term, debris flow, he used instead with appropriate descriptive adjectives when specifics are required. (Pierson and Costa 1987, 10)

FIGURE 3-36 Debris avalanches are larger, extremely rapid, Dry sand flow in often open-slope flows [Figure 3-34(b)]. The Mt. Columbia River Huascaran avalanche in (Figure 3-41) valley; dry sand involved 50 million m3 to 100 million in 3 of rock, from upper : ice, snow, and soil that traveled at velocities of as flowed through . much as 100 rn/sec. In this case, steam and air cush- notch in cliffs of . . .- more compact were suggested to account for the high veloc- sand and silt below ity and long distance of the debris travel (Varnes (Varnes 1978, 1978, 21). However, the contributions of snow and Figure 2.24). ice to the movement should also be considered. Landslide Types and Processes 67

FIGURE 3-37 Shallow dry sand flow along shore ffil of Lake Roosevelt, Washington State; wave erosion or saturation of sediment by lake water caused thin - . skin of material to -.'-- lose support and 5. -.- ravel off slope, - - ----. - - - - - formed on older -- terrace deposit -.. L . [Varnes 1978, Figure 2.25 (modified from ------;i- - Jones etal. 1961)].

According to Varnes, bedrock flows include 9. LANDSLIDE PROCESSES

"The processes involved in slope movements com- spatially continuous deformation and surficial prise a continuous series of events from cause to as well as deep creep. . . . [They involve] effect" (Varnes 1978, 26). In some cases, it may be extremely slow and generally nonaccelerating FIGURE 3-38 of differential movements among relatively intact more economical to repair the effects a landslide Old debris flow in units. Movements may (1) be along many shear than to remove the cause; a highway on the crest altered volcanic surfaces that are apparently not connected; (2) of a slope may be relocated rather than armoring rocks west of result in folding, bending, or bulging; or (3) the toe of the slope to prevent further erosion. Pahsimeroi River in south central roughly simulate those of viscous in dis- However, the design of appropriate, cost-effective remedial measures still requires a clear under- (Shaller tribution of velocities. (Varnes 1978, Figure 1991, Figure 8). 2.1, V) standing of the processes that are causing the land- COF'YIUGI IT slide. Although this understanding may require a JOl-IN S. SHELTON All the examples given by Varnes (1978) and reproduced as Figure 3-42 show movements that may have been initiated by sliding on the bedding or schistosity of the rock mass. These might all then be classified as complex slides. Further study may define the complex modes of movement to which these examples belong, in which sliding is followed by buckling (Hu and Cruden 1993). Clearly, further examples of ledwck uluw t1iould be explored in more detail before they can be more than tentatively classified. A is a debris flow from a . The flow mobilizes the loose accumulations of tephra (air- borne solids erupted from the volcano) on the volcano's slopes. Water for the flow may come from the ejection of crater lakes, condensations of erupted steam, the nucleation of water vapor on erupted particles and its , and the melting of snow and ice accumulated on a suffi- ciently high volcanic cone (Voight 1990). 68 Landslides: Investigation and Mitigation

FIGURE 3-39 No Concentration by Weight, C(%) Continuous spectrum of 99 91 80 5040 20 9.1 5.0 sediment 0.99 2.8 r- concentrations from sediment-laden Debris Flow to debris flows Mayflower Gulch o Streamflow (Eephemeral) - (modified from FO Wet Concrete Wright Hutchinson 1988,

Figure 15). Surprise Canyon _(Lw).w for G=2.60 - 2.75 — SAT — 1.wG Rio Reventado

Puerco (E)

River (E)

e Colorado River (E)

River

wRuver

Mu df low "(Rpl bris FIc Hyper

Chung River White Extreme Ri1 Grande River 1.0 I 1 10 100 1,000 10,000

Water Content, w (%) so

detailed site investigation, a reconnaissance of the landslide as soon as possible after its occurrence can allow important observations of the processes involved. These observations may guide both the FIGURE 3-40 site investigation and the remedial measures. Very rapid debris Although Vames (1978) provided a list of the flow, or debris causes of slides, the aims in this section are less avalanche, at ambitious. The section follows Varnes's distinction Franconia Notch, that the three broad types of landslide processes are New Hampshire, those that June 24, 1948, after several days of heavy rainfall. Increase shear stresses (Section 9.1), Colluvial soil up to Contribute to low strength (Section 9.2), and 5 m thick moved Reduce material strength (Section 9.3). down over bedrock along 450 m of a Common landslide triggering mechanisms are dis- 45-degree slope. cussed at greater length in Chapter 4. Levees appear at Processes and characteristics that contribute lateral margins. Flow covered US-3 to landslides are summarized in a checklist of land- (foreground) slide causes arranged in four practical groups ac- (Varnes 1978, cording to the and procedures necessary to Figure 2.17). begin the investigation (see p. 70). Ground causes Landslide Types and Processes

FIGURE 3-41 (top) NEVADO HUANDOY NEVADO HUASCARAN May31, 1970, 6395m NORTH PEAK SOUTH PEAK 6663m 6767m Huascaran debris ' A avalanche (Peru) GLACIAL'JV originated at Point A. Yungay had been // yPPDu-ERALANCA. \i protected from '•'' r' January 10, 1962, debris avalanche by ridge up to 240 m ___._. high (Point B), but •.: .. k // Area apparently overridden portion of later by avalanche debris but left undisturbed suggesting air avalanche over- cushioning effect topped protective W (_ ridge. Cemetery Hill (Point C) was only E safe place in Yungay, some 93 people escaping to it before Ro1 avalanche devastated surrounding area. Moving at an average speed of 320 km/hr, debris arrived at Point D on Rio Santa 14.5 km down 1 5-degree average slope within 3 to 4 min after can be identified with the customary tools of site starting from north reconnaissance and investigation. Changes in site peak of Huascaran morphology over time are apparent from the study (PointA). Debris of surveys, maps, and aerial photographs. Identi- flowed 2.5 km up fication of causes of movement requires the col- Rio Santa (Point E) and continued 160 lection of data over time from a variety of field km downstream to instruments, including seismographs, gauges, Pacific , flow gauges, and . Some changes in devastating villages material and mass properties with time may, how- and crops on its ever, be inferred from gradual changes in the mass floodplain [Varnes properties with distance. Anthropogenic causes 1978, Figure 2.27 can be documented by site records, plans, or other (modified from Magnosit Cluff 1971)]. observations.

9.1 Increased Shear Stresses

Shear stresses can be increased by processes that lead to removal of lateral support, by the imposi- tion of surcharges, by transitory stresses resulting from or earthquakes, and by uplift or tilting of the land surface. FIGURE 3-42 Examples of rock 9.1.1 Removal of Support flows [Varnes 1978, Figure 2.1p1l The toe of a slope can be removed by erosion, steep- (Nemok et al. 1972; ening the slope. Typical agents are streams and Zischinsky 1966)]. 70 Landslides: Investigation and Mitigation

material at depth within the displacing mass Checklist of Landslide Causes results in its extrusion or, if the base of the spread 1. Geological causes has liquefied, in its outward flow. These issues as Weak materials they relate to landslides in sensitive clay deposits Sensitive materials Weathered materials are discussed in Chapter 24. Sheared materials Jointed or fissured materials 9.1.2 Imposition of Surcharges Adversely oriented mass discontinuity The addition of material can result in increases of (bedding, schistosit etc.) Adversely oriented structural discontinuity both the length and the height of the slope. Water (fault, unconformity, contact, etc.) can be added by precipitation, both rain and snow; Contrast in permeability by the flow of surface and into the Contrast in stiffness (stiff, dense material displacing mass; and even by the growth of gla- over plastic materials) ciers. Surcharges can be added by the movement 2. Morphological causes of landslides onto the slope, by volcanic activity, Tectonic or volcanic uplift and by the growth of vegetation. Anthropogenic Glacial rebound surcharges include construction of fills, stockpiles, Fluvial erosion of slope toe Wave erosion of slope toe and waste dumps; structural weight; and water Glacial erosion of slope toe from leaking , systems, , Erosion of lateral margins sewers, and septic tanks. Subterranean erosion (solution, piping) Deposition loading slope or its crest 9.1.3 Transitory Stresses Vegetation removal (by fire, ) The local stress field within a slope can be greatly 3. Physical causes changed by transitory stresses from earthquakes Intense rainfall and explosions (both anthropogenic and vol- Rapid snow melt canic). Smaller transitory changes in the stress Prolonged exceptional precipitation field can result from and from Rapid drawdown (of and tides) activity such as pile driving and the passage of Earthquake Volcanic eruption heavy . Thawing Freeze-and-thaw weathering 9.1.4 Uplift or Tilting Shrink-and-swell weathering Uplift or tilting may be caused by tectonic forces 4. Human causes Excavation of slope or its toe or by volcanic processes. In either case, this type Loading of slope or its crest of increased may be associated with Drawdown (of reservoirs) earthquakes, which themselves can trigger land- slides (Section 9.1.3). The melting of the exten- Irrigation sive Pleistocene ice sheets has caused widespread uplift in temperate and circumpolar regions. Artificial Uplift of an area of the earth's surface generally Water leakage from utilities causes steepening of slopes in the area as drainage responds by increased incision. The cutting of val- leys in the uplifted area may cause valley rebound rivers, , and currents, and slope move- and accompanying fracturing and loosening of val- ments. Anthropogenic landslides can be caused by ley walls with inward shear along flat-lying dis- excavations for cuts, , pits, and canals, and continuities. The fractures and shears may allow by the drawdown of lakes and reservoirs. the buildup of pore-water pressures in the loosened Removal of material from the lateral margins of mass and eventually lead to landsliding. the displaced mass can also cause movement. Material can be removed from below the landslide 9.2 Low Strength by solution in terrain, by piping (the trans- port of sediment in groundwater flows), or by mm- Low strength of the earth or rock materials that irg. In some spreads, the loss of strength of the make up a landslide may reflect inherent material Landslide Types and Processes 71 characteristics or may result from the presence of effective intergranular pressure and frjction and discontinuities within the soil or rock mass. destroys capillary tension.

9.2.1 Material Characteristics 10. SUMMARY Materials may be naturally weak or may become weak as a result of common natural processes such In the initial reconnaissance of a landslide, the as saturation with water. Organic materials and activity and the materials displaced in that type of clays have low natural strengths. Rocks that have landslide would be described using terms from decomposed to clays by chemical weathering Table 3-2, the dimensions defined in Table 3-4 (weathered volcanic tuffs, schists, and serpen- would be estimated, and some preliminary hypoth- tinites, for example) develop similar properties. eses would be chosen about the causes of the Besides the of the individual particles of movements. A simple landslide report form is pro- which the material is composed, the arrangement vided in Figure 3-9; its format would allow the cre- of these particles (the fabric of the material) may ation of simple data bases suited to much of the cause low material strengths. Sensitive materials, data-base management software now available for which lose strength when disturbed, generally personal computers. The information collected have loose fabrics or textures. could be compared with summaries of other land- slides (WP/WLI 1991) and used to guide addi- 9.2.2 Mass Characteristics tional investigations and mitigative measures. Further investigation would increase the precision The soil or rock mass may be weakened by discon- of estimates of the dimensions and increase confi- tinuities such as faults, bedding surfaces, foliations, dence in the descriptions of activity and material cleavages, joints, fissures, shears, and sheared zones and in the hypotheses about the causes of move- (Chapters 12 and 14). Contrasts in bedded sedi- ment. The new information would then be added mentary sequences—such as stiff, thick beds over- to the data base to influence the analysis of new lying weak, plastic, thin beds or permeable sands landslides. These data bases could form the foun- (or sandstones) alternating with weak, imperme- dations of expert systems for . able clays (or shales)—are sources of weakness.

9.3 Reduced REFERENCES

Clays are particularly prone to weathering pro- ABBREVIATIONS cesses and other physicochemical reactipns. Hy- dration of clay minerals results in loss of cohesion, IAEG International Association of Engineering a process often associated with softening of fissured Geology clays. Fissuring of clays may be due to drying or to UNESCO United Nations Educational, Scientific, and release of vertical and lateral restraints by erosion Cultural Organization or excavation. The exchange of ions within clay WP/WLI Working Party on the World Landslide minerals with those in the pore water of the clays Inventory (International Geotechnical Societies and UNESCO) may lead to substantial changes in the physical properties of some clays. Electrical potentials set Abele, G. 1974. Bergsturze in den Alpen: ihre up by these chemical reactions or by other pro- Verbreitung, Morphologie und Folgeerscheinun- cesses may attract water to the weathering front. gen. Wissenschaftliche Alpenvereinshefte, Heft 25, The effects of extremes of caused Munchen. by severe are not confined to clays. Rocks Andrus, R.D., and T.L. Youd. 1987. SubsuTface In- may disintegrate under cycles of freezing and vestigation of a Liquefaction Induced Lateral Spread, thawing or thermal expansion and contraction. Thousand Springs Valley, Idaho. Miscellaneous Dry weather may cause desiccation cracking of GL-87-8. .S. Army Engineer Waterways weak or weathered rock along preexisting discon- Station, Vicksburg, Miss. tinuities, such as bedding planes. Wet weather Baars, D. 1989. Canyonlands Country: Geology of may dissolve natural rock that hold par- Can yonlands and National Parks. Canon ticles together. Saturation with water reduces Publishers Ltd., Lawrence, Kans., 140 pp. 72 Landslides: Investigation and Mitigation

Bagnold, R.A. 1956. The Flow of Cohesionless Crozier, M.J. 1984. Field Assessment of Slope Insta- Grains in Fluids. Proceedings of the Royal Society of bility. In Slope Instability (D. Brunsen and D.B. London, Vol. A249, pp. 235-297. Prior, eds.), John Wiley & Sons, , Barlow, W. 1888. On the Horizontal Movements of pp. 103-142. Rocks and the Relation of These Movements to Crozier, M.J. 1986. Landslides: Causes, Consequences, the Formation of Dykes and Faults and to Denuda- and Environment. Croom Helm, London, 252 pp. tion and the Thickening of Strata. Quarterly Jour- Cruden, D.M. 1978. Discussion of Hocking's Paper. nal of the Geological Society, Vol. 44, pp. 783-796. International Journal of and Mining Bates, R.L., and J.A. Jackson, eds. 1987. Glossary of Science, Vol. 15, No. 4, p. 217. Geology. American Geological Institute, Falls Cruden, D.M. 1984. More Rapid Analysis of Rock Church, Va., 788 pp. Slopes. Canadian Geotechnical Journal, Vol. 21, Bell, D.H., ed. 1992. Proc., Sixth International Sym- No. 4, pp. 678-683. posium on Landslides. A.A. Balkema, Rotterdam, Cruden, D.M. 1986. Discussion of Carter, M., and Netherlands, 2 vols., 1495 pp. S.P. Bentley. 1985. The Geometry of Slip Surfaces Beyer, W. H., ed. 1987. Handbook of Mathematical Beneath Landslides: Predictions from Surface Sciences, 6th ed. CRC Press, Inc., Boca Raton, Measurements. Canadian Geotechnical Journal, Florida, 860 pp. Vol. 23, No. 1, p. 94. Bishop, A.W. 1973. Stability of Tips and Spoil Heaps. Cruden, D.M. 1991. A Simple Definition of a Quarterly Journal of , Vol. 6, Landslide. Bulletin of the International Association No. 4, pp. 335-376. of Engineering Geology, No. 43, pp. 27-29. Bonnard, C., ed. 1988. Proc., Fifth International Sym- Cruden, D.M., Z.Q. Hu, and Z.Y. Lu. 1993. Rock posium on Landslides. A.A. Balkema, Rotterdam, Topples in the Highway Cut West of Clairvivaux Netherlands, 3 vols., 1564 pp. Creek, Jasper, Alberta. Canadian Geotechnical Brabb, E.E., and B.L. Harrod, eds. 1989. Landslides: Journal, Vol. 30, No. 6, pp. 1016-1023. Extent and Economic Significance: Proc., 28th In- Cruden, D.M., S. Thomson, and B.A. Hoffman. ternational Geological Congress: Symposium on 1991. Observations of Graben Geometry in Land- Landslides, A.A. Balkema, Rotterdam, Nether- slides. In Slope Stability Engineering-Developments lands, 385 pp. and Applications: Proc., International Conference on Brown, W.M., D.M. Cruden, andJ.S. Denison. 1992. Slope Stability, , 15-18 April (R.J. The Directory of the World Landslide Inventory. Chandler, ed.), Thomas Telford Ltd., London, U.S. Geological Survey Open File Report 92-427, pp. 33-36. 2l6pp. Dana, J.D. 1877. New Text-book of Geology Designed Brunsden, D. 1984. Mudslides. In Slope Instability (D. for Schools and Academies. Ivison, Blakeman, Brunsden and D.B. Prior, eds.), John Wiley and Taylor, New York, 366 pp. Sons, Chichester, U.K., Chap. 9, pp. 363-418. De Freitas, M.H., and R.J. Watters. 1973. Some Field Brunsden, D., and D.B. Prior, eds. 1984. Slope In- Examples of Toppling Failure. Geotechnique, Vol. stability. John Wiley and Sons, Chichester, U.K., 23, No. 4, pp. 495-5 14. 62Opp. Eckersley, J.D. 1990. Instrumented Laboratory Flow- Canadian Geotechnical Society. 1984. Proc., Fourth slides. Geotechnique, Vol. 40, No. 3, pp. 489-502. International Symposium on Landslides. Toronto, Eisbacher, G.H., and J.J. Clague. 1984. Desrructive Canada, 3 vols., 1484 pp. Mass Movements in High Mountains: Hazard and Church, H.K. 1981. Excavation Handbook. McGraw- Management. Paper 84-16. Geological Survey of Hill, New York, N.Y., 1024 pp. Canada, Ottawa, , 230 pp. Cluff, L.S. 1971. Peru Earthquake of May 31, 1970: Eliot, T.S. 1963. Collected Poems 1909-1962. Faber, Engineering Geology Observations. Bulletin of the London, 234 pp. Seismological Society of America, Vol. 61, No. 3, Engineering News Record. 1971. Contrived Landslide pp. 511-521. Kills 15 in . Vol. 187, p. 18. Costa, J.E., and G.E Wieczorek, eds. 1987. Debris Evans, S.G., J.J. Clague, G.J.Woodsworth, and 0. Flows/Avalanches: Process, Recognition, and Mitiga- Hungr. 1989. The Pandemonium Creek Rock tion. Reviews in Engineering Geology, Vol. 7, Avalanche, British Columbia. Canadian Geotech- Geological Society of America, , ., nical Journal, Vol. 26, No. 3, pp. 427-446. 239 pp. Giraud, A., L. Rochet, and P. Antoine. 1990. Cross, W. 1924. Historical Sketch of the Landslides of Processes of Slope Failure in Crystallophyllian the Gaillard Cut. Memoir 18. National Academy Formations. Engineering Geology, Vol. 29, No. 3, of Sciences, Washington, D.C., pp. 22-43. pp. 241-253. Landslide Types and Processes 73

Goodman, R.E., and J.W. Bray. 1976. Toppling of Hutchinson, J.N. 1967. The Free Degradation of Rock Slopes. In Proc., Specialty Conference on Cliffs. In Proc., Geotechnical Confer- Rock Engineering for Foundations and Slopes, ence on Shear Strength Properties of Nat,ural Soils and Boulder, Cob., Aug. 15-18, American Society of Rocks, Norwegian Geotechnical Institute, Oslo, Civil Engineers, New York, Vol. 2, pp. 201-234. Vol. 1, pp. 113-118. Haefeli, R. 1965. Creep and Progressive Failure in Hutchinson, J.[N.] 1968. Mass Movement. In En- Snow, Soil, Rock, and Ice. In Proc., Sixth Interna- cyclopedia of (R.W. Fairbridge, ed.), tional Conference on and Foundation Reinhold, New York, pp. 688-695. Engineering, University of Toronto Press, Vol. 3, Hutchinson, J.N. 1973. The Response of London pp. 134-148. Clay Cliffs to Differing Rates of Toe Erosion. Geo- Hansen, W.R. 1965. Effects of the Earthquake of March logia Applicata e Idrogeologia, Vol. 8, pp. 22 1-239. 27, 1964, at Anchorage, . U.S. Geological Hutchinson, J.N. 1983. Methods of Locating Slip Survey Professional Paper 542-A, 68 pp. Surfaces in Landslides. Bulletin of the International Harrison, J.V., and N.L. Falcon. 1934. Collapse Association of Engineering Geology, Vol. 20, No.3, Structures. Geological Magazine, Vol. 71, No. 12, pp. 235-252. pp. 529-539. Hutchinson, J.N. 1988. General Report: Morpholog- Harrison, J.V., and N.L. Falcon. 1936. Gravity Col- ical and Geotechnical Parameters of Landslides in lapse Structures and Mountain Ranges as Exemp- Relation to Geology and . In Proc., lified in South-western Persia. Quarterly Journal Fifth International Symposium on Landslides (C. of the Geological Society of London, Vol. 92, Bonnard, ed.), A.A. Balkema, Rotterdam, Nether- pp. 9 1-102. lands, Vol. 1, pp. 3-35. Heim, A. 1932. Bergsturz und Menschenleben. Hutchinson, J.N. 1991. Periglacial and Slope Processes. Beiblatt zur Vierteljahrsschrift der Naturforschenden Engineering Geology Special Publication 7, Geo- Gesellschaft in Zurich, Vol. 77, pp. 1-217. Trans- logical Society of London, pp. 283-33 1. lated by N. Skermer under the title Landslides Hutchinson, J.N., and R.K. Bhandari. 1971. Un- and Human Lives, BiTech Publishers, Vancouver, drained Loading, a Fundamental Mechanism of British Columbia, 1989, 195 pp. Mudflows and Other Mass Movements. Geo- Hocking, G. 1976. A Method for Distinguishing technique, Vol. 21, pp. 353-358. Between Single and Double Plane Sliding of Hutchinson, J.N., and T.P. Gostelow. 1976. The De- Tetrahedral Wedges. International Journal of Rock velopment of an Abandoned Cliff in London Clay Mechanics and Mining Science, Vol. 13, No. 7, at Hadleigh, Essex. Philosophical Transactions of the pp. 225-226. Royal Society of London, Series A, Vol. 283, pp. Hoek, E., and J.W. Bray. 1981. Rock Slope Engineering. 557-604. Institution of Mining and , London, IAEG Commission on Landslides. 1990. Suggested 358 pp. Nomenclature for Landslides. Bulletin of the Inter- Horswill, P., and A. Horton. 1976. Cambering and national Association of Engineering Geology, No. 41, Valley Bulging in the Gwash Valley at Emping- pp. 13-16. ham, Rutland. Philosophical Transactions of the Jones, FO., D.R. Embody, and W.L. Peterson. 1961. Royal Society of London, Series A, Vol. 283, No. Landslides Along the Columbia River Valley, North- 1315, pp. 427-462. eastern Washington. U.S. Geological Survey Pro- Hsu, K.J. 1975. Catastrophic Debris Streams (Sturz- fessional Paper 367, 98 pp. stroms) Generated by . Bulletin of the Jordan, R.H. 1949. A Florida Landslide. Journal of Geological Society of America, Vol. 86, No. 1, Geology, Vol. 57, No. 4, pp. 418-419. pp. 129-140. Keefer, D.K., and A.M. Johnson. 1983. : Hu, X.Q., and D.M. Cruden. 1993. Buckling Defor- Morphology, Mobilization and Movement. U.S. Geo- mation in the , Alberta. Canadian logical Survey Professional Paper 1264, 56 pp. Geotechnical Journal, Vol. 30, No. 2, pp. 276-286. Kostak, B., and D.M. Cruden. 1990. The Moire Huder, J. 1976. Creep in Bundner . Norwegian Crack Gauges on the Crown of the Frank Slide. Geotechnical Institute (Laurits Bjerrum Memorial Canadian Geotechnical Journal, Vol. 27, No. 6, Volume), Oslo, pp. 125-153. pp. 835-840. Hungr, 0., and S.G. Evans. 1988. Engineering Eval- Kovari, K., and P;Fritz. 1984. Recent Developments uation of Fragmental . In Proc., in the Analysis and Monitoring of Rock Slopes. Fifth International Symposium on Landslides (C. In Proc., Fourth International Symposium on Land- Bonnard, ed.), A.A. Balkema, Rotterdam, Neth- slides, Canadian Geotechnical Society, Toronto, erlands, Vol. 1, pp. 685-690. Vol. 1, pp. 1-16. 74 Landslides: Investigation and Mitigation

Kozlovskii, E.A. (ed.). 1988. Landslides and Mudflows. Flows. In Debris Flows/Avalanches: Process, Recog- UNESCO-UNEP, Moscow, 2 vols., 376 pp. nition, and Mitigation (I.E. Costa and G.E Wie- Krahn, J., and N.R. Morgenstern. 1979. The Ulti- czorek, eds.), Reviews in Engineering Geology, Vol. mate Frictional Resistance of Rock Discon- 7, Geological Society of America, Boulder, Cob., tinuities. International Journal of Rock Mechanics pp. 1-12. and Mining Science, Vol. 16, No. 2, pp. 127-133. Potter, D.B., and G.E. McGill. 1978. Valley Anti- Kyunttsel, V.V. 1988. Landslides. In Landslides and dines of the Needles District, Canyonlands Mudflows (E.A. Kozlovskii, ed.), United Nations National Park, Utah. Bulletin of the Geological Environment Programme, UNESCO, Moscow, Society of America, Vol. 89, No. 6, pp. 952-960. Vol. 1, pp. 35-54. Prior, D.B., N. Stephens, and D.R. Archer. 1968. McCalpin, J. 1984. Preliminary Age Classification of Composite Mudflows on the Antrim of Landslides for Inventory Mapping. In Proc., 21st North-East Ireland. Geografiska Annaler, Vol. Engineering Geology and Soils Engineering Sym- 50A, No. 2, pp. 65-78. posium, University of Idaho, Moscow, pp. 99-120. Radbruch-Hall, D.H. 1978. Gravitational Creep of McConnell, R.G., and R.W. Brock. 1904. Report on Rock Masses on Slopes. In Rockslides and Ava- the Great Landslide at Frank, Alberta. In Annual lanches (B. Voight, ed.), Vol. 1: Natural Pheno- Report for 1903, Department of the Interior, mena, Elsevier, Amsterdam, Netherlands, pp. Ottawa, Canada, Part 8, 17 pp. 607-657. McGill, G.E., and A.W. Stromquist. 1979. The Radbruch-Hall, D.H., D.J. Varnes, and W.Z. Savage. Grabens of Canyonlands National Park, Utah: 1976. Gravitational Spreading of Steep-Sided Geometry, Mechanics, and Kinematics. Journal of Ridges ("sackung") in Western United States. Geophysical Research, Vol. 84, No. B9, pp. 4547- Bulletin of the International Association of Engi- 4563. neering Geology, No. 14, pp. 23-35. McRoberts, E.C., and N.R. Morgenstern. 1974. Ramsay, J.G. 1967. Folding and Fracturing of Rocks. Stability of Slopes in Frozen Soil, Mackenzie McGraw-Hill, New York, 568 pp. Valley, North West Territories. Canadian Geo- Ritchie, A.M. 1963. Evaluation of Rockfall and Its technical Journal, Vol. 11, No. 4, pp. 554-573. Control. In Highway Research Record 17, HRB, Morgenstern, N.R. 1985. Geotechnical Aspects of National Research Council, Washington, D.C., Environmental Control. In Proc., 11th Interna- pp. 13-28. tional Conference on Soil Mechanics and Foundation Rybár, J., and J. Dobr. 1966. Fold Deformations in the Engineering, A.A. Balkema, Rotterdam, Nether- North-Bohemian Coal Basins. Sbornik geologickych lands, Vol. 1, pp. 155-185. v ed, Rada HIG, No. 5, pp. 133-140. Mueller, L. 1964. The Rock Slide in the Vaiont Shaller, P.J. 1991. Analysis of a Large, Moist Land- Valley. Rock Mechanics and Engineering Geology, slide, Lost River Range, Idaho, U.S.A. Canadian Vol. 2, No. 3-4, pp. 148-212. Geotechnical Journal, Vol. 28, No. 4, pp. 584-600. Nemok, A., J. Pasek, and J. Rybár. 1972. Classifi- Shelton, J.S. 1966. Geology illust-rated. W.H. Freeman cation of Landslides and Other Mass Movements. and Co., San Francisco, 434 pp. Rock Mechanics, Vol. 4, pp. 7 1-78. Shreve, R.L. 1968. The Blackhawk Landslide. Special Nicoletti, P.G., and M. Sorriso-Valvo. 1991. Geo- Paper 108. Geological Society of America, morphic Controls of the Shape and Mobility of Boulder, Cob., 47 pp. Rock Avalanches. Bulletin of the Geological Society Shroder, J.F. 1971. Landslides of Utah. Bulletin 90. of America, Vol. 103, No. 10, pp. 1365-1373. Utah Geological and Mineralogical Survey, 50 pp. Ostaficzuk, S. 1973. Large-Scale Landslides in North- Skempton, A.W. 1970. First-TIme Slides in Over- western Libya. Acta Geologica Pcilonica, Vol. 23, Consolidated Clays. Geotechnique, Vol. 20, No. 3, No. 2, pp. 23 1-244. pp. 320-324. Palmer, L. 1977. Large Landslides of the Columbia Skempton, A.W., and J.N. Hutchinson. 1969. Sta- River Gorge, and Washington. In Land- bility of Natural Slopes and Embankment Foun- slides (D.R. Coates, ed.), Reviews in Engineering dations. In Proc., Seventh International Conference Geology, Vol. 3, Geological Society of America, on Soil Mechanics and Foundation Engineering, Boulder, Cob., pp. 69-83. Sociedad Mexicana de Mecána de Suebos, Panet, M. 1969. Discussion of K.W. John's Paper , State of the Art Volume, pp. 29 1-340. (ASCE Proc. Paper 5865, March 1968). Journal of Skempton, A.W., and A.G. Weeks. 1976. The the Soil Mechanics and Foundation Division, ASCE, History of the Lower Vol. 95, No. SM2, pp. 685-686. and Weald Clay Vale near Sevenoaks, Pierson, T.C., and J.E. Costa. 1987. A Rheologic Kent. Philosophical Transactions of the Royal Society Classification of Subaerial Sediment—Water of London, Series A, Vol. 283, pp. 493-526. Landslide Types and Processes 75

Swaminathan, C.G., ed. 1980. Proc., Third Interna- Varnes, H.D. 1949. Landslide Problems of Southwest- tional Symposium on Landslides, Santa Prakashan, ern Colorado. U.S. Geological Survey Circular 31, New Delhi, India, 3 vols., 927 pp. 13 pp. Tavenas, F., J.Y. Chagnon, and P. LaRochelle. 1971. Voight, B. 1990. The 1985 Volcano The Saint-Jean Vianney Landslide: Observations Catastrophe: Anatomy and Retrospection. Journal and Eyewitness Accounts. Canadian Geotechnical of Volcanology and Geothermal Research, Vol. 44, Journal, Vol. 8, No. 3, pp. 463-478. No. 1-2, pp. 349-386. Ter-Stepanian, G. 1980. Measuring Displacements of Walton, G., and T. Atkinson. 1978. Some Geo- Wooded Landslides with Trilateral Signs. In Proc., technical Considerations in the Planning of Sur- Third International Symposium on Landslides (C.G. face Coal Mines. Transactions of the Institution of Swaminathan, ed.), Santa Prakashan, New Delhi, Mining and Metallurgy, Vol. 87, pp. A147-A171. India, Vol. 1, pp. 355-36 1. Ward, W.H. 1948. A Coastal Landslip. In Proc., Terzaghi, K. 1950. Mechanism of Landslides. In Second International Conference on Soil Mechanics Application of Geology to Engineering Practice and Foundation Engineering, International Society (S. Paige, ed.), Geological Society of America, of Soil Mechanics and Foundation Engineering, New York, pp. 83-1 23. Rotterdam, Vol. 2, pp. 33-38. Terzaghi, K., and R.B. Peck. 1948. Soil Mechanics in Wieczorek, G.F. 1984. Preparing a Detailed Engineering Practice. John Wiley & Sons, New Landslide-Inventory Map for Hazard Evaluation York, 566 pp. and Reduction. Bulletin of the Association of En- Thomson, S., and D.W. Hayley. 1975. The Little gineering Geologists, Vol. 21, No. 3, pp. 337-342. Smoky Landslide. Canadian Geotechnical Journal, Wilson, S.D. 1970. Observational Data on Ground Vol. 12, No. 3, pp. 379-392. Movements Related to Slope Instability. Journal of Van Gassen, W., and D.M. Cruden. 1989. Momen- the Soil Mechanics and Foundations Division, ASCE, tum Transfer and Friction in the Debris of Rock Vol. 96, No. SM4, pp. 152 1-1544. Avalanches. Canadian Geotechnical Journal, Vol. Wilson, S.D., and P.E. Mikkelsen. 1978. Field 26, No. 4, pp. 623-628. Instrumentation. In Special Report 176: Landslides: Van Horn, R. 1975. Largest Known Landslide of Its Analysis and Control (R.L. Schuster and R.J. Type in the United States-A Failure by Lateral Krizek, eds.), TRB, National Research Council, Spreading in Davis County, Utah. Utah Geology, Washington, D.C., pp. 112-138. Vol. 2, pp. 82-87. WP/WLI. 1990. A Suggested Method for Reporting Varnes, D.J. 1958. Landslide Types and Processes. In a Landslide. Bulletin of the International Association Special Report 29: Landslides and Engineering Prac- of Engineering Geology, No.41, pp. 5-12. tice (E.B. Eckel, ed.), HRB, National Research WP/WLI. 1991. A Suggested Method for a Landslide Council, Washington, D.C., pp. 20-47. Summary. Bulletin of the International Association of Varnes, D.J. 1978. Slope Movement Types and Pro- Engineering Geology, No. 43, pp. 101-110. cesses. In Special Report 176: LAndslides: Analysis WP/WLI. 1993a. A Suggested Method for Describ- and Control (R.L. Schuster and R.J. Krizek, eds.), ing the Activity of a Landslide. Bulletin of the Inter- TRB, National Research Council, Washington, national Association of Engineering Geology, No.47, D.C., pp. 11-33. pp. 53-57. Varnes, D.J. 1984. Landslide Hazard Zonation: A WP/WLI. 1993b. Multilingual Landslide Glossary. Bi- Review of Principles and Practice. UNESCO, Paris, Tech Publishers, Richmond, British Columbia, 63 pp. Canada, 59 pp. Varnes, D.J., D.H. Radbruch-Hall, and W.Z. Savage. Zaruba, Q., and V. Mend. 1969. Landslides and Their 1989. Topographic and Structural Conditions in Control, 1st ed. Elsevier, Amsterdam, Netherlands, Areas of Gravitational Spreading of Ridges in the 205 pp. Western United States. U.S. Geological Survey Zaruba, Q., and V. Mend. 1982. Landslides and Their Professional Paper 1496, 28 pp. Control, 2nd ed. Elsevier, Amsterdam, Nether- Varnes, D.J., D.H. Radbruch-Hall, K.L. Varnes, W.K. lands, 324 pp. Smith, and W.Z. Savage. 1990. Measurements of Zischinsky, U. 1966. On the Deformation of High Ridge-Spreading Movements (Sackungen) at Bald Slopes. In Proc., First Congress of the International , Lake County, Colorado, 1975- Society for Rock Mechanics, Lisbon, Sept. 25-1 1989. U.S. Geological Survey Open File Report Oct., 1966, International Society for Rock 90-543, 13 pp. Mechanics, Lisbon, Portugal, Vol. 2, pp. 179-185.