Precise Determination of Geoid Height and Free-Air Gravity Anomaly at Syowa Station, Antarctica

Total Page:16

File Type:pdf, Size:1020Kb

Precise Determination of Geoid Height and Free-Air Gravity Anomaly at Syowa Station, Antarctica Earth Planets Space, 51, 159–168, 1999 Precise determination of geoid height and free-air gravity anomaly at Syowa Station, Antarctica Kazuo Shibuya, Koichiro Doi, and Shigeru Aoki Center for Antarctic Environment Monitoring, National Institute of Polar Research, Kaga 1-9-10, Itabashi-ku, Tokyo 173-8515, Japan (Received July 1, 1998; Revised December 14, 1998; Accepted December 15, 1998) From the International Terrestrial Reference Frame 1994 (ITRF94) coordinates of the Doppler Orbitography Radiopositioning Integrated by Satellites (DORIS) beacon marker at Syowa Station (69.0◦S, 39.6◦E), Antarctica, we derived the ellipsoidal height of the Scientific Committee on Antarctic Research (SCAR) Global Positioning System (GPS) point as 42.240 m on the World Geodetic System 1984 (WGS84) associated ellipsoid of a tide free Earth at the epoch of 1993.0. Because the SCAR GPS reference mark was 21.165 m above the local mean sea level at the epoch of 1993.0, and because the sea surface topography is estimated as −1.29 m, the ground data of geoid height can be estimated as 22.37 m on the WGS84 ellipsoid. As for error estimate of the above value, 20–30 cm formal error can be assigned including 3 cm error from the DORIS determination, 1 cm error from the local geodetic tie, and the dominant 20–30 cm error from uncertain modeling of sea surface topography, etc. The EGM96 geoid model gives the synthetic geoid height of 22.10 m at Syowa Station; the discrepancy of 27 cm from the observed value is within the 36 cm cumulative (to the degree 360) rms (root-mean-square) error of the model. We retried similar determination at Breid Bay (70.2◦S, 23.8◦E) and made a tie to the inland outcropped Seal Rock; the obtained value of 21.4 m has an overall error of 1.8 m. These ground data can be used as test data for generating higher- order (n, m ≥ 360) geopotential models. With the establishment of the International Absolute Gravity Basestation Network (IAGBN) standard value at Syowa Station and gravimetric connection to the Seal Rock, ground data of free-air gravity anomalies of 0.05 mgal accuracy at Syowa Station and 1 mgal accuracy at Seal Rock were obtained. These gravity ground data will also serve as test data for adjusting the satellite- and/or shipborne-derived gravity anomaly maps in the region concerned. 1. Introduction ephemeris NNSS (Navy Navigation Satellite System) po- Determination of an accurate geoid model in the Antarc- sitioning result and make the tie to the inland Seal Rock tic region is important to study global geodynamics of the No. 25-01 geodetic mark in East Dronning Maud Land. With atmosphere/ocean and solid-earth interaction. Before GPS these accurate geoid height data and the estimated elevation (Global Positioning System) development, only satellite above sea level, the gravity measurements were re-analyzed Doppler positioning was practically applicable in the to obtain free-air gravity anomalies after adjustment to the In- marginal sea ice zone of Antarctica to obtain the ground data ternational Absolute Gravity Basestation Network (IAGBN; of geoid height. The attained accuracy was 4 m, restricted Boedecker and Fritzer, 1986) Syowa Station standard value. by the uncertainty of broadcast ephemeris positioning (e.g. the obtained value of 16.8 m at Breid Bay (70.2◦S, 23.8◦E); Shibuya et al., 1991). Today, combined use of GPS and other 2. DORIS Determined Coordinates of the Beacon space geodetic techniques enables us to estimate rather pre- Marker at Syowa Station cise geoid height in Antarctica, and we present a result of Figure 1 illustrates Syowa Station which is located on East 20–30 cm accuracy ground data obtained at Syowa Station Ongul Island of L¨utzow-Holm Bay, Antarctica. There are (69.0◦S, 39.6◦E). four reference marks by different space geodetic techniques, The most convenient positioning in the Antarctic region, namely satellite Doppler point A which is identical to the that is, GPS positioning is based on the WGS84 (World classic astronomical station, DORIS (Doppler Orbitography Geodetic System 1984; Defense Mapping Agency, 1987) by Radiopositioning Integrated by Satellites) beacon point geocentric coordinate system. Since the WGS84 reference D, SCAR (Scientific Committee on Antarctic Research) GPS frame usually applies the ellipsoid with the semi-major campaign point G which is identical to the classic geodetic axis a = 6378137.0 m and the flattening factor 1/f = control point No. 23-16, and the VLBI (Very Long Base- 298.2572235630, we hereafter call the associated ellipsoid line Interferometry) reference point R at the 11 m S/X band as the WGS84 ellipsoid and place the final result on it. We paraboloid antenna. All these four reference marks are in also re-determine ground data at Breid Bay with a precise bedrock area. According to Boucher et al. (1996; Table T7), ITRF94 (International Terrestrial Reference Frame 1994) coordinates Copy rightc The Society of Geomagnetism and Earth, Planetary and Space Sciences (SGEPSS); The Seismological Society of Japan; The Volcanological Society of Japan; of the DORIS beacon marker (Photo 1) at the epoch of 1993.0 The Geodetic Society of Japan; The Japanese Society for Planetary Sciences. were obtained as 159 160 K. SHIBUYA et al.: PRECISE DETERMINATION OF GEOID HEIGHT AND FREE-AIR GRAVITY ANOMALY Fig. 1. Syowa Station is located on East Ongul Island of Lutzow-Holm¨ Bay, Antarctica (left). There are four reference marks by different space geodetic techniques around the main facilities (right). All the four reference marks are in bedrock area. As for explanation of the abbreviated marks and facilities, see text. that Eq. (1) is given in the tide free system (C. Boucher, 1997; personal communication). −→ Kanao et al. (1995) estimated the offset vector DG as −→ DG = (−316.322 m, 62.323 m, −73.692 m) (2) by combined use of two-frequency GPS relative position- ing and classic geodetic surveying within an overall error of 1 cm. Thus the DORIS-determined ITRF94 coordinates of the SCAR GPS point were estimated as XG,DORIS = 1766498.873 − 316.322 = 1766182.551 m, YG,DORIS = 1460274.430 + 62.323 = 1460336.753 m, (3) ZG,DORIS =−5932211.730 − 73.692 =−5932285.422 m. 3. WGS84 Coordinates of the SCAR GPS Point in a Tide Free System It is well known that the WGS84 coordinate system has a slight inconsistency against the ITRF coordinate system (e.g. Abusali et al., 1995), and we apply a summary of seven parameter transformations by Tobita (1997) to convert Eq. (3) into the WGS84 coordinate values: X 0.078 −8 Photo 1. DORIS beacon pier installed near the Earth Science Laboratory Y = −0.505 + (1.0 − 1.01 × 10 ) (ESL; see Fig. 1) of Syowa Station. Z −0.253 WGS84 1 δω −δψ X · −δω 1 δε Y , (4) δψ −δε 1 Z ITRF94 XD = 1766498.873 m, YD = 1460274.430 m, (1) where δω =−3.394 × 10−8, δψ = 1.454 × 10−9 and Z =−5932211.730 m, D δε =−8.872 × 10−8 are given as the rotational parame- with an uncertainty of 3 cm for each coordinate. It is noted ters. It is noted that δω in the original formula of McCarthy K. SHIBUYA et al.: PRECISE DETERMINATION OF GEOID HEIGHT AND FREE-AIR GRAVITY ANOMALY 161 Fig. 2. Sea surface topography around Syowa Station in the region bounded by (0◦–60◦E, 60◦S–75◦S) after the degree 20 expansion model as part of the EGM96 geoid modeling (Lemoine et al., 1997). Contour interval is 10 cm. Calculated based on the information from the NIMA (National Imagery and Mapping Agency) web site. (1992) has opposite sign. Application of Eq. (4) to Eq. (3) 1992), Odamaki et al. (1991) indicate apparent sea level fall and subsequent transformation into the WGS84 geodetic co- with a rate of 1.0 cm/year. From Eqs. (5) and (5), we estimate ordinates results in hNo. 23-16 = dh + hBM1040 + (apparent rise) φ = ◦ . ,λ= ◦ . , G 69 00 24 600 S G 39 35 06 152 E ∼ 18.816 m + 2.338 m + 0.01 m = 21.16 m (6) (4 ) HG = 42.240 m at the epoch of 1993.0. at the epoch of 1993.0. The uncertainty of the seven param- eters in Eq. (4) may introduce about 2 cm uncertainty into 5. Obtained Ground Data of Geoid Height at Syowa Station the ellipsoidal height HG of Eq. (4 ). It is noted that local mean sea level is not identical to the global geoid surface, and sea surface topography has 4. Reduction to the Local Mean Sea Level to be corrected for in order to estimate the geoidal undula- In East Ongul Island, there is a leveling route in the form tion. For example, Rapp et al. (1991) modeled the sea sur- of a closed loop from the bench mark BM1040 at the tide face topography ζ for the global ocean using the GEOSAT gauge station of Syowa Station (Fig. 1), which passes through data. An improved sea surface topography expanded to de- the No. 23-16 geodetic mark, that is, the SCAR GPS point. gree and order 20 is now available from the information at Several Japanese Antarctic Research Expeditions (JARE-23, the web site http://cddis.gsfc.nasa.gov/egm96/general info/ -33 and -37) repeated a first-order leveling survey within the readme.sst egm96 topex ers1, and Fig. 2 illustrates the cal- closure error of 3 mm, and the height difference between the culated 0.1 m model contours around Lutzow-Holm¨ Bay. We bench mark BM1040 and the SCAR GPS point, h, at the obtain ζ at Syowa Station as epoch of 1992.0 was obtained as ζSYO =−1.29 m.
Recommended publications
  • It Is Quite Common for Confusion to Arise About the Process Used During a Hydrographic Survey When GPS-Derived Water Surface
    It is quite common for confusion to arise about the process used during a hydrographic survey when GPS-derived water surface elevation is incorporated into the data as an RTK Tide correction. This article explains a little about the process. What we are discussing here might be a tide-related correction to a chart datum for coastal surveying – maybe to update navigational charts, or it might be nothing to do with tides at all. For example, surveying a river with the need to express bathymetry results as a bottom elevation on the desired vertical datum – not simply as “depth” results. Whether it is anything to do with tidal forces or not, the term “RTK Tide” is ubiquitous in hydrographic-speak to refer to vertical corrections of echo sounding data using RTK GPS. Although there is some confusing terminology, it’s a simple idea so let’s try to keep it that way. First keep in mind any GPS receiver will give the user basically two things in terms of vertical positioning: height above the GPS reference ellipsoid surface and height above Mean Sea Level (MSL) where ever he or she is on the Earth. How is MSL defined? Well, a geoid surface is a measure of the strength of gravity which in turn mostly controls the height of the sea; it is logical to say that MSL height equals the geoid height and vice versa. Using RTK techniques to obtain tide information is a logical extension of this basic principle. We are measuring the GPS receiver height above a geoid.
    [Show full text]
  • Shaded Elevation Map of Ohio
    STATE OF OHIO DEPARTMENT OF NATURAL RESOURCES DIVISION OF GEOLOGICAL SURVEY Ted Strickland, Governor Sean D. Logan, Director Lawrence H. Wickstrom, Chief SHADED ELEVATION MAP OF OHIO 0 10 20 30 40 miles 0 10 20 30 40 kilometers SCALE 1:2,000,000 427-500500-600600-700700-800800-900900-10001000-11001100-12001200-13001300-14001400-1500>1500 Land elevation in feet Lake Erie water depth in feet 0-6 7-12 13-18 19-24 25-30 31-36 37-42 43-48 49-54 55-60 61-66 67-84 SHADED ELEVATION MAP This map depicts the topographic relief of Ohio’s landscape using color lier impeded the southward-advancing glaciers, causing them to split into to represent elevation intervals. The colorized topography has been digi- two lobes, the Miami Lobe on the west and the Scioto Lobe on the east. tally shaded from the northwest slightly above the horizon to give the ap- Ridges of thick accumulations of glacial material, called moraines, drape pearance of a three-dimensional surface. The map is based on elevation around the outlier and are distinct features on the map. Some moraines in data from the U.S. Geological Survey’s National Elevation Dataset; the Ohio are more than 200 miles long. Two other glacial lobes, the Killbuck grid spacing for the data is 30 meters. Lake Erie water depths are derived and the Grand River Lobes, are present in the northern and northeastern from National Oceanic and Atmospheric Administration data. This digi- portions of the state. tally derived map shows details of Ohio’s topography unlike any map of 4 Eastern Continental Divide—A continental drainage divide extends the past.
    [Show full text]
  • Meyers Height 1
    University of Connecticut DigitalCommons@UConn Peer-reviewed Articles 12-1-2004 What Does Height Really Mean? Part I: Introduction Thomas H. Meyer University of Connecticut, [email protected] Daniel R. Roman National Geodetic Survey David B. Zilkoski National Geodetic Survey Follow this and additional works at: http://digitalcommons.uconn.edu/thmeyer_articles Recommended Citation Meyer, Thomas H.; Roman, Daniel R.; and Zilkoski, David B., "What Does Height Really Mean? Part I: Introduction" (2004). Peer- reviewed Articles. Paper 2. http://digitalcommons.uconn.edu/thmeyer_articles/2 This Article is brought to you for free and open access by DigitalCommons@UConn. It has been accepted for inclusion in Peer-reviewed Articles by an authorized administrator of DigitalCommons@UConn. For more information, please contact [email protected]. Land Information Science What does height really mean? Part I: Introduction Thomas H. Meyer, Daniel R. Roman, David B. Zilkoski ABSTRACT: This is the first paper in a four-part series considering the fundamental question, “what does the word height really mean?” National Geodetic Survey (NGS) is embarking on a height mod- ernization program in which, in the future, it will not be necessary for NGS to create new or maintain old orthometric height benchmarks. In their stead, NGS will publish measured ellipsoid heights and computed Helmert orthometric heights for survey markers. Consequently, practicing surveyors will soon be confronted with coping with these changes and the differences between these types of height. Indeed, although “height’” is a commonly used word, an exact definition of it can be difficult to find. These articles will explore the various meanings of height as used in surveying and geodesy and pres- ent a precise definition that is based on the physics of gravitational potential, along with current best practices for using survey-grade GPS equipment for height measurement.
    [Show full text]
  • A Fast Method for Calculation of Marine Gravity Anomaly
    applied sciences Article A Fast Method for Calculation of Marine Gravity Anomaly Yuan Fang 1, Shuiyuan He 2,*, Xiaohong Meng 1,*, Jun Wang 1, Yongkang Gan 1 and Hanhan Tang 1 1 School of Geophysics and Information Technology, China University of Geosciences, Beijing 100083, China; [email protected] (Y.F.); [email protected] (J.W.); [email protected] (Y.G.); [email protected] (H.T.) 2 Guangzhou Marine Geological Survey, China Geological Survey, Ministry of Land and Resources, Guangzhou 510760, China * Correspondence: [email protected] (S.H.); [email protected] (X.M.); Tel.: +86-136-2285-1110 (S.H.); +86-136-9129-3267 (X.M.) Abstract: Gravity data have been playing an important role in marine exploration and research. However, obtaining gravity data over an extensive marine area is expensive and inefficient. In reality, marine gravity anomalies are usually calculated from satellite altimetry data. Over the years, numer- ous methods have been presented for achieving this purpose, most of which are time-consuming due to the integral calculation over a global region and the singularity problem. This paper proposes a fast method for the calculation of marine gravity anomalies. The proposed method introduces a novel scheme to solve the singularity problem and implements the parallel technique based on a graphics processing unit (GPU) for fast calculation. The details for the implementation of the proposed method are described, and it is tested using the geoid height undulation from the Earth Gravitational Model 2008 (EGM2008). The accuracy of the presented method is evaluated by comparing it with marine shipboard gravity data.
    [Show full text]
  • THE EARTH's GRAVITY OUTLINE the Earth's Gravitational Field
    GEOPHYSICS (08/430/0012) THE EARTH'S GRAVITY OUTLINE The Earth's gravitational field 2 Newton's law of gravitation: Fgrav = GMm=r ; Gravitational field = gravitational acceleration g; gravitational potential, equipotential surfaces. g for a non–rotating spherically symmetric Earth; Effects of rotation and ellipticity – variation with latitude, the reference ellipsoid and International Gravity Formula; Effects of elevation and topography, intervening rock, density inhomogeneities, tides. The geoid: equipotential mean–sea–level surface on which g = IGF value. Gravity surveys Measurement: gravity units, gravimeters, survey procedures; the geoid; satellite altimetry. Gravity corrections – latitude, elevation, Bouguer, terrain, drift; Interpretation of gravity anomalies: regional–residual separation; regional variations and deep (crust, mantle) structure; local variations and shallow density anomalies; Examples of Bouguer gravity anomalies. Isostasy Mechanism: level of compensation; Pratt and Airy models; mountain roots; Isostasy and free–air gravity, examples of isostatic balance and isostatic anomalies. Background reading: Fowler §5.1–5.6; Lowrie §2.2–2.6; Kearey & Vine §2.11. GEOPHYSICS (08/430/0012) THE EARTH'S GRAVITY FIELD Newton's law of gravitation is: ¯ GMm F = r2 11 2 2 1 3 2 where the Gravitational Constant G = 6:673 10− Nm kg− (kg− m s− ). ¢ The field strength of the Earth's gravitational field is defined as the gravitational force acting on unit mass. From Newton's third¯ law of mechanics, F = ma, it follows that gravitational force per unit mass = gravitational acceleration g. g is approximately 9:8m/s2 at the surface of the Earth. A related concept is gravitational potential: the gravitational potential V at a point P is the work done against gravity in ¯ P bringing unit mass from infinity to P.
    [Show full text]
  • The Global Positioning System the Global Positioning System
    The Global Positioning System The Global Positioning System 1. System Overview 2. Biases and Errors 3. Signal Structure and Observables 4. Absolute v. Relative Positioning 5. GPS Field Procedures 6. Ellipsoids, Datums and Coordinate Systems 7. Mission Planning I. System Overview ! GPS is a passive navigation and positioning system available worldwide 24 hours a day in all weather conditions developed and maintained by the Department of Defense ! The Global Positioning System consists of three segments: ! Space Segment ! Control Segment ! User Segment Space Segment Space Segment ! The current GPS constellation consists of 29 Block II/IIA/IIR/IIR-M satellites. The first Block II satellite was launched in February 1989. Control Segment User Segment How it Works II. Biases and Errors Biases GPS Error Sources • Satellite Dependent ? – Orbit representation ? Satellite Orbit Error Satellite Clock Error including 12 biases ? 9 3 Selective Availability 6 – Satellite clock model biases Ionospheric refraction • Station Dependent L2 L1 – Receiver clock biases – Station Coordinates Tropospheric Delay • Observation Multi- pathing Dependent – Ionospheric delay 12 9 3 – Tropospheric delay Receiver Clock Error 6 1000 – Carrier phase ambiguity Satellite Biases ! The satellite is not where the GPS broadcast message says it is. ! The satellite clocks are not perfectly synchronized with GPS time. Station Biases ! Receiver clock time differs from satellite clock time. ! Uncertainties in the coordinates of the station. ! Time transfer and orbital tracking. Observation Dependent Biases ! Those associated with signal propagation Errors ! Residual Biases ! Cycle Slips ! Multipath ! Antenna Phase Center Movement ! Random Observation Error Errors ! In addition to biases factors effecting position and/or time determined by GPS is dependant upon: ! The geometric strength of the satellite configuration being observed (DOP).
    [Show full text]
  • Geographical Influences on Climate Teacher Guide
    Geographical Influences on Climate Teacher Guide Lesson Overview: Students will compare the climatograms for different locations around the United States to observe patterns in temperature and precipitation. They will describe geographical features near those locations, and compare graphs to find patterns in the effect of mountains, oceans, elevation, latitude, etc. on temperature and precipitation. Then, students will research temperature and precipitation patterns at various locations around the world using the MY NASA DATA Live Access Server and other sources, and use the information to create their own climatogram. Expected time to complete lesson: One 45 minute period to compare given climatograms, one to two 45 minute periods to research another location and create their own climatogram. To lessen the time needed, you can provide students data rather than having them find it themselves (to focus on graphing and analysis), or give them the template to create a climatogram (to focus on the analysis and description), or give them the assignment for homework. See GPM Geographical Influences on Climate – Climatogram Template and Data for these options. Learning Objectives: - Students will brainstorm geographic features, consider how they might affect temperature and precipitation, and discuss the difference between weather and climate. - Students will examine data about a location and calculate averages to compare with other locations to determine the effect of geographic features on temperature and precipitation. - Students will research the climate patterns of a location and create a climatogram and description of what factors affect the climate at that location. National Standards: ESS2.D: Weather and climate are influenced by interactions involving sunlight, the ocean, the atmosphere, ice, landforms, and living things.
    [Show full text]
  • A Seamless Vertical-Reference Surface for Acquisition, Management and Display (Ecdis) of Hydrographic Data
    SEAMLESS VERTICAL DATUM A SEAMLESS VERTICAL-REFERENCE SURFACE FOR ACQUISITION, MANAGEMENT AND DISPLAY (ECDIS) OF HYDROGRAPHIC DATA A report prepared for the Canadian Hydrographic Service under Contract Number IIHS4-122 David Wells Alfred Kleusberg Petr Vanicek Department of Geodesy and Geomatics Engineering University of New Brunswick PO. Box 4400 Fredericton, New Brunswick Canada E3B 5A3 FINAL REPORT (DRAFT) November 22, 2004 Page 1 SEAMLESS VERTICAL DATUM Final Report 15 July 1995 FINAL REPORT (DRAFT) November 22, 2004 Page 2 SEAMLESS VERTICAL DATUM TABLE OF CONTENTS Table of contents...........................................................................................................................2 Executive summary.......................................................................................................................5 Acronyms used in this report ........................................................................................................6 1. Introduction...............................................................................................................................8 1.1 Problem statement.......................................................................................................8 1.2 The role of vertical-reference surfaces in navigation..................................................8 1.3 Vertical-reference surface accuracy issues..................................................................9 1.3.1 Depth measurement errors .........................................................................10
    [Show full text]
  • Detection of Caves by Gravimetry
    Detection of Caves by Gravimetry By HAnlUi'DO J. Cmco1) lVi/h plates 18 (1)-21 (4) Illtroduction A growing interest in locating caves - largely among non-speleolo- gists - has developed within the last decade, arising from industrial or military needs, such as: (1) analyzing subsUl'face characteristics for building sites or highway projects in karst areas; (2) locating shallow caves under airport runways constructed on karst terrain covered by a thin residual soil; and (3) finding strategic shelters of tactical significance. As a result, geologists and geophysicists have been experimenting with the possibility of applying standard geophysical methods toward void detection at shallow depths. Pioneering work along this line was accomplishecl by the U.S. Geological Survey illilitary Geology teams dUl'ing World War II on Okinawan airfields. Nicol (1951) reported that the residual soil covel' of these runways frequently indicated subsi- dence due to the collapse of the rooves of caves in an underlying coralline-limestone formation (partially detected by seismic methods). In spite of the wide application of geophysics to exploration, not much has been published regarding subsUl'face interpretation of ground conditions within the upper 50 feet of the earth's surface. Recently, however, Homberg (1962) and Colley (1962) did report some encoUl'ag- ing data using the gravity technique for void detection. This led to the present field study into the practical means of how this complex method can be simplified, and to a use-and-limitations appraisal of gravimetric techniques for speleologic research. Principles all(1 Correctiolls The fundamentals of gravimetry are based on the fact that natUl'al 01' artificial voids within the earth's sUl'face - which are filled with ail' 3 (negligible density) 01' water (density about 1 gmjcm ) - have a remark- able density contrast with the sUl'roun<ling rocks (density 2.0 to 1) 4609 Keswick Hoad, Baltimore 10, Maryland, U.S.A.
    [Show full text]
  • Accuracy of Flight Altitude Measured with Low-Cost GNSS, Radar and Barometer Sensors: Implications for Airborne Radiometric Surveys
    sensors Article Accuracy of Flight Altitude Measured with Low-Cost GNSS, Radar and Barometer Sensors: Implications for Airborne Radiometric Surveys Matteo Albéri 1,2,* ID , Marica Baldoncini 1,2, Carlo Bottardi 1,2 ID , Enrico Chiarelli 3, Giovanni Fiorentini 1,2, Kassandra Giulia Cristina Raptis 3, Eugenio Realini 4, Mirko Reguzzoni 5, Lorenzo Rossi 5, Daniele Sampietro 4, Virginia Strati 3 and Fabio Mantovani 1,2 ID 1 Department of Physics and Earth Sciences, University of Ferrara, Via Saragat, 1, 44122 Ferrara, Italy; [email protected] (M.B.); [email protected] (C.B.); fi[email protected] (G.F.); [email protected] (F.M.) 2 Ferrara Section of the National Institute of Nuclear Physics, Via Saragat, 1, 44122 Ferrara, Italy 3 Legnaro National Laboratory, National Institute of Nuclear Physics, Via dell’Università 2, 35020 Legnaro (Padova), Italy; [email protected] (E.C.); [email protected] (K.G.C.R.); [email protected] (V.S.) 4 Geomatics Research & Development (GReD) srl, Via Cavour 2, 22074 Lomazzo (Como), Italy; [email protected] (E.R.); [email protected] (D.S.) 5 Department of Civil and Environmental Engineering (DICA), Polytechnic of Milan, Piazza Leonardo da Vinci 32, 20133 Milano, Italy; [email protected] (M.R.); [email protected] (L.R.) * Correspondence: [email protected]; Tel.: +39-329-0715328 Received: 7 July 2017; Accepted: 13 August 2017; Published: 16 August 2017 Abstract: Flight height is a fundamental parameter for correcting the gamma signal produced by terrestrial radionuclides measured during airborne surveys.
    [Show full text]
  • TOPOGRAPHIC MAP of OKLAHOMA Kenneth S
    Page 2, Topographic EDUCATIONAL PUBLICATION 9: 2008 Contour lines (in feet) are generalized from U.S. Geological Survey topographic maps (scale, 1:250,000). Principal meridians and base lines (dotted black lines) are references for subdividing land into sections, townships, and ranges. Spot elevations ( feet) are given for select geographic features from detailed topographic maps (scale, 1:24,000). The geographic center of Oklahoma is just north of Oklahoma City. Dimensions of Oklahoma Distances: shown in miles (and kilometers), calculated by Myers and Vosburg (1964). Area: 69,919 square miles (181,090 square kilometers), or 44,748,000 acres (18,109,000 hectares). Geographic Center of Okla- homa: the point, just north of Oklahoma City, where you could “balance” the State, if it were completely flat (see topographic map). TOPOGRAPHIC MAP OF OKLAHOMA Kenneth S. Johnson, Oklahoma Geological Survey This map shows the topographic features of Oklahoma using tain ranges (Wichita, Arbuckle, and Ouachita) occur in southern contour lines, or lines of equal elevation above sea level. The high- Oklahoma, although mountainous and hilly areas exist in other parts est elevation (4,973 ft) in Oklahoma is on Black Mesa, in the north- of the State. The map on page 8 shows the geomorphic provinces The Ouachita (pronounced “Wa-she-tah”) Mountains in south- 2,568 ft, rising about 2,000 ft above the surrounding plains. The west corner of the Panhandle; the lowest elevation (287 ft) is where of Oklahoma and describes many of the geographic features men- eastern Oklahoma and western Arkansas is a curved belt of forested largest mountainous area in the region is the Sans Bois Mountains, Little River flows into Arkansas, near the southeast corner of the tioned below.
    [Show full text]
  • Pilot's Operating Handbook and Faa
    FEBRUARY 2006 VOLUME 33, NO. 2 The Official Membership Publication of The International Comanche Society The Comanche Flyer is the official monthly member publication of the Volume 33, No. 2 • February 2006 International Comanche Society www.comancheflyer.com 5604 Phillip J. Rhoads Avenue Hangar 3, Suite 4 Bethany, OK 73008 Published By the International Comanche Society, Inc. Tel: (405) 491-0321 Fax: (405) 491-0325 CONTENTS www.comancheflyer.com 2 Letter From The President Karl Hipp ICS President Karl Hipp Cover Story: Comanche Spirit Tel: (970) 963-3755 4 Mike and Pattie Adkins – Kim Blonigen E-mail: [email protected] Pilots, Partners and Owners of N4YA Managing Editor 6 2005-2006 ICS Board of Directors Kim Blonigen & Tribe Representatives E-mail: [email protected] 6 2005-2006 ICS Standing Advertising Manager Committees & Chairpersons John Shoemaker 6 ICS 2006 Nominating Committee 800-773-7798 Fax: (231) 946-9588 6 ICS Website Update E-mail: [email protected] Special Feature Graphic Design 8 Surviving Katrina Koren Herriman 9 Call for Nominees E-mail: [email protected] Pilot Pointers Printer Village Press 10 It Should Not Happen To You — Omri Talmon 2779 Aero Park Drive Comanche Accidents for Traverse City, MI 49685-0629 November 2005 and a Case www.villagepress.com Technically Speaking Office Manager 14 Online Intelligence — Gaynor Ekman Learning to Use the Garmin 430 and 530 Tel: (405) 491-0321 17 Technical Tidbits Michael Rohrer Fax: (405) 491-0325 E-mail: [email protected] 19 CFF-Approved CFIs The Comanche Flyer is available to members; From the Logbook the $25 annual subscription rate is included in the Society’s Annual Membership dues in 20 Transatlantic Adventures – Part Two Karl Hipp & US funds below.
    [Show full text]