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Conference on Applied Statistics in Agriculture 1989 - 1st Annual Conference Proceedings
STATISTICAL ISSUES IN STUDIES OF THERMOREGULATION IN FARM ANIMALS
A. M. Parkhurst
G. L. Hahn
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Recommended Citation Parkhurst, A. M. and Hahn, G. L. (1989). "STATISTICAL ISSUES IN STUDIES OF THERMOREGULATION IN FARM ANIMALS," Conference on Applied Statistics in Agriculture. https://doi.org/10.4148/ 2475-7772.1449
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STATISTICAL ISSUES IN STUDIES OF THERMOREGULATION IN FARM ANIK~LS
A. M. Parkhurst and G. L. Hahn University of Nebraska-Lincoln
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U. S. Meat Animal Research Center, ARS-USDA, Clay Center, NE Abstract Patterns of tympanic temperature response were identified in ad-lib-fed cattle exposed to constant or cyclic (±7 C) conditions at two levels of air temperature: 10 C and 28 C. Use of time series analysis following the DDS approach of Pandit and Wu indicate the thermoregulatory control dynamics for steers at 28±7 C were markedly different from those at the other conditions. Preliminary evaluations using the ideas of chaos and non-linear dynamics show promise of further characterization of stress responses in farm animals.
Keywords: circadian rhythms, tympanic temperatures, data dependent systems, time series, entrainment, chaos theory, non-linear dynamics, thermal stress
1. Background of Biological Investigation The capability of farm animals to maintain homeothermy through thermoregulation is central to coping with thermal stressors through behavioral or physiological responses. Typical behavioral responses include seeking a more favorable microclimate if available (e.g., shelter from wind or precipitation in cold, or shade from sun and increased utilization of water in hot environments), and altering posture and contacts with other animals to change exposed surface area. Decreased feed intake lowers metabolic heat production and therefore decreases the amount of heat dissipation required in hot weather, while increased feed intake in cold conditions leads to higher metabolic rates. Physiological responses include adjustment of metabolic levels necessary to sustain body processes, vasodilation and increased respiration to increase heat dissipation, or vasoconstriction to conserve body heat. Minimizing the overall impact of thermal stressors is essential to satisfactory performance, health and welfare of farm animals. Variations are cornmon among species and individuals in their ability to adjust to thermal challenges. Disruptions of normal body temperature and thermoregulatory processes can be important criteria for assessing the ability of farm animals to cope with thermal stressors. Thermoregulatory control is a complex process linked primarily to the hypothalamus in the brain. In thermoregulatory studies of animals, body temperature, along with other physiological, environmental and behavioral variables, is observed at regular time intervals. Such time series usually exhibit cyclic fluctuations which are thought by many investigators to be circadian in nature (Aschoff, 1983; Stanier et al., 1984; Hahn, 1988). While much remains to be learned about thermoregulatory control systems in mammals (Cossins and Bowler, 1987), recent evidence indicates an innate monophasic body temperature rhythm in ad-lib-fed animals in the absence of stressors (Hahn, 1988). These innate rhythms, with maxima in late evening and minima in mid-morning, can be altered by environmental stressors (e.g., adverse air temperature, weather events, or transport). Shifts in the mean, amplitude and phase of the circadian body temperature rhythms occur when thermal thresholds characteristic of species and individual animals are exceeded.
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Bos well-known off (i.e. order analyzing cycles, initial real linear to U. linear Priestley, body Conference on Applied Statistics in Agriculture in der more (Strogatz discussed turn as in roots, core combinations time-series S. properties the and or represent taurus when responses evaluation rhythm sys characterized Pulses Pol and also terms Meat to differential memory" over monogastric marked temperature controlled Hahn, combination rhythms on data. terns stressors. assumption difference Hence, basically by (baseline) have model equations a positive, the both when rhythms growing may second Cossins thermal a Animal of of 1988). in 1987). may 1987; model (DDS) than wide been more Low of Kansas State University that and 0.5 and the the the the the the be of in of be a Conference on Applied Statistics in Agriculture Kansas State23 University may reflect sinusoidal dynamics with different degrees of damping. Real roots with absolute value close to one can represent constant trend of growth or decay while complex roots close to III may represent circadian rhythms with the period given by the imaginary part. 3. Description of Pilot Controlled-Environment Study Measurements: Tympanic temperatures were recorded hourly by a datalogger from thermocouple sensors inserted into the ear canal of each steer, using techniques previously described (Wiersma and Stott, 1973; Scott et al., 1973). The overall system was carefully calibrated, with obtained accuracy limi ts of .05 C or better. Considerable effort was required to maintain functioning sensors because of breakage, disconnected or chewed leads, and the need to alternate sensors from ear to ear at no more than weekly intervals to minimize ear canal irritation. However, the technique does provide an acceptable index of hypothalamic temperature (Benzinger, 1959, 1964; Guidry and McDowell, 1965; Weirsma and Stott, 1974), which serves as the principal integrator from which animals adjust heat production, loss or retention to maintain thermoregulatory control by animals (Stanier et al., 1984). Treatments: The treatment design was a 2 x 2 factorial consisting of two factors: regime and temperature. The two temperature levels selected represented non- stressing (thermoneutral, 10 C) and potentially stressing (hot, 28 C) conditions, based on prior reports on the effects of temperature on cattle performance and physiological response (c.f., NRC, 1981). Regime levels selected were cyclic and constant temperatures. Cyclic conditions sinusoidally varied ±7 C about either of the mean temperature levels, to approximate naturally-varying spring/fall (thermoneutral) or summer (hot) conditions. Constant conditions represent a contrasting environment often used in environmental research as a basis for comparison. Experiment: In this study, four animals were housed in pairs and each pair received two treatments. All four animals began the study at the non stressing temperature. Two of the steers were placed in the constant temperature regime; the other two, in the cyclic regime. Steers were kept in a thermoneutral environment for two weeks, with tympanic temperatures recorded the last eight days. The steers were then subjected to heat stress and the experiment continued for six days. During the experiment, the steers were maintained in individual stalls in controlled-environment chambers at MARC with a photoperiod of 14h light and 10h dark. They were ad-lib-fed a high-energy pelleted ration, supplemented with 1 kg hay/day to maintain rumen function. 4. Statistical Analysis The analysis focuses on identifying patterns of response over time. Resul ts are used to support assumptions proposed in the literature as reviewed above and/or to generate new constructs or models for thermoregulatory systems. Visual inspection of the time series data indicates a dynamic process (Figure 1 ) and because of the suspected heterogeneity among animals, data from each steer were analyzed separately. Individual analyses were also made for each treatment, since the parameters of interest were more likely to remain constant wi thin rather than between the treatment segments. In addition, a 24h washout period was imposed between the thermoneutral and thermal stress conditions, with measurements at the beginning of the thermal stress conditions omitted from the analyses in an attempt to eliminate New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 https://newprairiepress.org/agstatconference/1989/proceedings/4 New Prairie Press 24 possible but process. roots phase stressor. rhythm. cyclic of physiological (1,1) (2n,2n-l) to each environmental resul chamber can may as to may component sinusoidal thermal individual secondary detect revealing feedback (Steer thermoregulatory thermoneutral literature Perhaps is x(t+i) univariate search or thermoneutral Phase critical the attractor of limit is At DDS Using a become After the The /1/, A dynamic imposed approximately momentum, illustrate take rather be phase damped ts animal, simple this to angle could diagrams cycle, analysis individual 219), periodicity? for where DDS Table interpreted information treatment by the transitory stress a a No the 2 control provided Under strategy entrained. portrait. high-order is (22%) is point, period as function The motion.) components days on chaos? discussed case, differentiating sinusoidal in such analysis problem via verify approach the as deterministic a (Figure i 2. stressor. process. indicated condition, the that i.e. state acclimation are biorhythm the closed is thermal well was to condition sinusoidal autoregression, composite system characteristic the the of models process animal's a it studied the be appears indicated effects characteristic to of the that a from is used The random 24h, The is as behavior The 3b). which above. ARMA of interest is brought of wave. trend estimate curve, time the the stress, The chaotic such signal, by to phase DDS requires not It Green's Figure cyclic did axes would Green's it to This to to is (6,5), and biorhythm. Green's function linearity compare fits of hot among function the is walk, delay. to innate procedure is Additional illustrating as a estimate reveal determine the the which Analysis back predominantly of of diagram start-up lies also natural could be the substantiates then 1. one a roots percent represent cyclic or well x(t) thermal function. thermal Table the the Table approximately function. dimensions thermostat. thermal Table brought Is function into roots The biorhythm the time not quasi-periodic; possible is might pairs is possible of phase constraints happen derivative with the vs. for were the indicates ~~en associated of the choice removed, period parameters conditions. 1. 3. so information condition. phase period it variation. stressor stress 1. which signal cyclic expect the acclimation of treatments. much order back it's time attractor. space takes detected. environmental the The (Figure when This But to (78%) ranged appears complex For to with other of of the 48h 2.5 in frequency series estimate relative may into first should the provides to the estimate thermal of on are that for roots the lag and approach the with the for the the noise influenced to ideas can may how 2) the most the from dynamics treatments, identify Consider phase the signal hot suggests to conjugate The does process (Attractors hot die However, order the derivative. is to analysis shows a innate be close be be model. Basically, does be time stress the importance cyclic periodic parsimonious cyclic ratio of a the variance counterintuitive. insight an Conference on Applied Statistics in Agriculture related proposed out. obtained cyclic impacts animals not leads with the entrained low versus the of parameters the to one environmental of amplitude series. rhythm. a (Moon, the the by appear too suggests result roots examination the heat This is Suppose order temperature stressor the was stationary /1/. vibrations the to are begin biorhythm treatment motion to a into with constant velocity to from large the models, for on of in useful In innate not stress system damped result a 1987). states by close model to study ARMA Such of each Kansas State University lag, The hot and for the the The the the the the the the the the an as be to or is a Conference on Applied Statistics in Agriculture Kansas State25 University close to the limit cycle of the internal biorhythm, the resulting periodic motion can become entrained at the stressor frequency. Thus, the conclusion of a sinusoidal function of period 24 for thermal stress treatment is reaffirmed. The phase diagrams for the other treatments suggest a different story. The attractor for the cyclic thermoneutral condition appears almost periodic or quasiperiodic, (Figure 3a). This could happen because the periodic force of the treatment is too small to become entrained and what is displayed is a combination of oscillators. For constant thermal stress, the attractor may be periodic, but, it is difficult to tell because the process rises to a threshold and then decreases, (Figure 3d). The most complex condition is the constant thermoneutral state, (Figure 3c). This process may also be quasiperiodic. It could be dominated by a combination of oscillators and the attractor could become strange suggesting a chaotic process. The above observations are also supported by the use of the Fourier spectrum (Figure 4). In each case, the peak at approximately 24h indicates a diurnal cycle. However, the multiharmonics in the neutral conditions suggest that is far from the whole story. These phenomena require further study and may be addressed by Poincare maps, surfaces in a three dimensional phase space or other tools used to identify routes to chaos (Berge et al., 1984; Moon, 1987). 5. Issues Generated by the Statistical Analysis The DDS approach involves a sequence of F tests, multiple t-tests, and tests for autocorrelation as statistical issues in estimating dimensionality. There are also issues of size of sampling intervals, length of series, magnitude of signal-to-noise ratio and statistical graphics needed to detect and illustrate treatment differences. There are questions about the robustness of the DDS procedure in modeling data with deterministic periodicity and trends. The concept of stochastic periodicity (Box and Jenkins, 1976) needs to be re-examined especially in light of chaos. And, since the characteristic roots are useful not only in detecting periodicity and trends, but also in interpreting Green's function, attention needs to be given to more conditional tests for eigenvalues. However, the most intriguing statistical issues raised in this paper are generated by consideration of chaos, the study of non-linear dynamic systems. Some rudimentary questions are: When is a system linear or nonlinear? Is the ability to differentiate among attractors dependent on the signal to noise ratio? Is it possible to distinguish among periodic, aperiodic or quasi~periodic,chaotic, and random events, especially in the presence of self-excited vibrations? Physicists, engineers and mathematicians are developing new ways to describe the dynamics of nonlinear systems. Statisticians need to respond with equally inventive ways of estimating those ever changing parameters (Priestley, 1988; Tong, 1983). 6. Further Considerations It may be fruitful to conceptualize thermoregulation in terms of non linear oscillators, such as those used in modeling human responses as mentioned above (Strogatz 1987) and in Glass and Mackey (1988). The primary oscillator(s) represents the animal's own biorhythm. In the thermoneutral zone, it is a self-excited function. It is not constrained by an external driving force. However, as the ambient temperature is increased, so is the amplitude of the external driving force(s) the secondary New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 https://newprairiepress.org/agstatconference/1989/proceedings/4 New Prairie Press 26 oscills.tor(s). over beyond drives stress. lmpact al., fractal to apparent control These the time 1984; the external of those processes analysis, potential Eventually, new as the system. Hayashi, the discussed conjectures external driving Thus, anims.l and and for Control a 1964; responses the generally such thermal in function behaviorally forCe. need impac'C this Moon, evaluations passes threshold paper. further of becomes the 1987; of from farm the study and to Thompson the The animals evaluation forcing dominant physiologically is further of internal theory reached. non-linear and to funcc:ion delineate and of stressors. by Stewart, self-excited In the chaos, techniques this dynamics copes itself second Conference on Applied Statistics in Agriculture thermoregulatory bifurcation situation, 1986), with is oscillator oscillator (Berge 'l>lhich dynarr;ic have thermal Kansas State University the or go et an Conference on Applied Statistics in Agriculture Kansas27 State University TABLES TABLE 1. Dimension of ARMA Model for each Treatment Sample 1 Sample 2 NEUTRAL STRESS NEUTRAL STRESS CYCLIC ( 4 , 3 ) (3 , 1) (6,5) (2,1) CONSTANT (1,1) ( 2 , 0) (2,0) (3,1) TABLE 2. Periods Indicated by Conjugate Roots of Length One Sample 1 Sample 2 NEUTRAL STRESS NEUTRAL STRESS CYCLIC 2.24* 24.58 23.70+ 24.90 CONSTANT * Coefficients not significant, (a = 1%) + Roots for autoregression and moving average cancel. - No roots of length one. TABLE 3 . Parameters of Stationary Process Temperature Tym12anic Chamber Sample 1 Sample 2 MEAN ( 0 C) 40.15 40.25 28.56 AMPLITUDE 0.97 0.87 6.37 PHASE ANGLE (rad. ) 2.44 2.48 1. 47 PHASE SHIFT (rad. ) -1.17 1.13 0.60 New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 https://newprairiepress.org/agstatconference/1989/proceedings/4 New Prairie Press 28 A Arrowsmith, Aschoff, Therm. Benzinger, Benzinger, temperature Berge, Experimental Box, a and Chapman Cossins, Finch, Life. Glass, Guidry, relevance Hahn, press) Joseph, Hahn, reassessment Hahn, indicating Rept. Biometeorologv University Hayashi, temperature Moon, rhythms l\'CR. and animals" Qualitative Deterministic Control. Engineers. G. 1981. Princeton G.L., F. B/A G. . G.L., Biology Pierre, L. V. & A. E. MO. . J. C. A. C. in L. Hall, for 4.4:320-323. and A. T. J. rapid P. T. Press, Nat'l. D. 1987. in A. 1983. fluctuations J. 1988. Biology R. Paper cattle 1964. Approach relative H. "Effect Holden-Day, production and 1986. and M. Yves man". H. 8:143-147. K H. & Approach London/New University A. John and 1959. changes Aerobiology. C. Parkhurst, and R. G. Research Princeton, Chaotic "Body 86-4009. Nienaber, "Circadian 1964. Pomeau Nonlinear 18:49-61. K. Hacke)'. E. wiley M. in Froc. of C. "Body with to "On McDowell. Jenkins. Bowler. to M. in in temperature environment selected in San Vibrations: "The and environmer:tal York. Press. & Council. Apolications. physical Nat'l. Turbulence. body the Place. temperature meat and New Sons, H. Francisco. 1988. C. control Oscillations American thermal tropics". REFERENCES J.A. C. temperature". Jersey. Vidal. animals". 1965 1987. 1976. Acad. Princeton, Kew 1982. environments". Klerncke, heat Nat'l. Nienaber. rhythms 0:1 From An of York. homeostasis Meteorological Sci. John Introduction in nutrie!lt "Tympanic 1984. influences". Time regulation bod)' Temperature Ordinary Chapman J. Clocks in beef Academy Amer. and 45:645-657. Wiley in !'iew Ani. Series Physical temperature: 1987. J. Order farm cattle: C. Jersey. to req'J.irements & membrane Sci. Dairy Soc. Differential & Press, of Hill, and L. Chaos: for Analysis: within Proc. Sons, animals "Tympanic Biology Society, man". SYstems. Cosc;. Agric. Biometeorologv the 62:531-542. Sci. Aupl It's Conference on Applied Statistics in Agriculture London/New Washington, New A temperature The sense Chaos: 8th i 49(1):74-77. Svmpos. review". ed 1986. of control York. Engrs. Forecasting of Boston, temperature Equations: a Rhythms Scientists Conf. Princeton of Animals. review domestic Towards York. "Body Soc. D.C. Kansas State University and MA for St. (In 1-: of on & Conference on Applied Statistics in Agriculture Kansas 29State University Pandit, S. M. and S. M. Wu. 1983. Time Series and Svstem Analvsis with Applications. John Wiley & Sons, New York. Parkhurst, A. M. and G. L. Hahn. 1987. "Data dependent systems time series analysis of cattle tympanic temperature rhythms". Amer. Soc. Agric. Engrs. St. Joseph, MO. Paper MCR 87-131. Priestley, M. B. 1988. Non-linear and Non-stationary Time Series Ana1vsis. Academic Press, San Diego, CA 92101. SAS Institute Inc. 1984. SAS/ETS User's Guide, Version 5 Edition. SAS Institute Inc., Cary, NC. Scott, 1. M., H. D. Johnson, and G. L. Hahn. 1983. "Effect of programmed diurnal temperature cycles on plasma thyroxine level, body temperature and feed intake of Holstein dairy cows". Int'l J. Biometeorology 7(1):47-62. Stanier, M. W., L. E. Mount, and J. Bligh. 1984. Energy Balance and Temperature Regulation. Cambridge Univ. Press, Cambridge. Strogatz, S. H. 1987. "A comparative analysis of models of the human sleep wake cycle". Lectures on Mathematics in the Life Sciences. American Mathematical Society. Providence 19:1-38. Thompson, J. M. T., and H. B. Stewart. 1986. Nonlinear Dynamics and Chaos: Geometrical Methods for Engineers and Scientists. John Wiley & Sons, New York. Tong, H. 1983. "Threshold models in non-linear time series analysis". Lecture Notes in Statistics Vol. 21. Springer-Verlag, New York. Wiersma, F. and G. H. Stott. 1974. "Dairy cow body temperatures in a hot climate". Trans. ASAE 17:745-747. Wiersma, F. and G. H. Stott. 1983. "A technique for securing a temperature probe adjacent to the tympanic membrane in bovine". Trans. ASAE 26(1):185- 187. New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 Conference on Applied Statistics in AgriculturewGo o Kansas State University Figure 1. Tympanic Temperature Sample 1 Sample 2 o o Steer -186--186 C c Steer 219 ·1212 12 < ·u· .,, :iii.1\. .tk , , "j - 11- '11 - _-,'i.,11 ,/~; \', ·t·,· -I .t ~J.\ ./.', .,., '1', X ·H· " x + ., '~;. :t .•+ ~ .;,... \ x ++ " .,, + " , " XX :+:. '\ , x +":Ii- ~.; + +t- + + + il 1 x·,x,· I,ll +. ,10'I()-- - )( +.t· 10 -- :tIt .. .~ ; ..t!~ X~ , \.\ .~-) + ...f t.~!1~-1 '; :J: ;:)( >4/ ~~ :x ·f Vi ., l .'/ ·.~ii\-1 x \:. ;;+ ~~~·i~~ -~.~!wa 'y~/ +1' "t+ ';§1.1 -u+ ,'~ .l 1t 't ~:I/,/ JD - " .tt " 3030· -I ~,ii. ,~~r 'I'~"", .•~~t .... ~..... 1: ·"-... ""!i. - .::t t t x ~II/.\? I~'I.I '/;I~ ., .tIUI"' I ",' .'I~ ·'I~ri;'r·I' '~/I~" .~; /~I!" II- ," )( .. ~ I) -1"):I"l'':'~i'':.i':;!;'I,'I:'': 37-1 ,__ _ 37 ------·--~------r---- -~I---- 37 -----'--1-I I , o lOO100 200 300 -.--- o :lOU o 100laO 200 300 Hours Hours o o ,," C Steer 1791~(9 C Steer 223 12 -- 12 + 11 ..)~:'+ 1~'~" t t + 111 j - -t:/l.... ~ ..... ~lth ..."\:~~ -~i'''. :1: .",•. , .. ,J.I!· .~•. .t 1~ .,. V·\ 10 - H},I () - ).:t ...... ,;l~'/'\'':'V''\,!",(, l' Xx (,(X ·11· ..,~' 39 3U -I,{;>;:~",~;:!t:: .•~':"!/I\:~+':~I1-;I· +.~;~ 1. )( -';V~:~l';·!fij.:~<1;:;1!J;il;;It.ftr~'~1~¥j~~/" ... ,. ..::1." ~ :t .,.+ *'* 30 - 3U:JIJ - :]'/-1:..1'1 ------r----·--·---l------l----~.-I 1 ,--- 37:n -1------~-----·---~·I-··------,------,--- ao 100 200 300 o 100 200 300 Hours Hours X recordedr6COrded datadtrtn notnat used In DOSDDS analysis +t recordedr6~::ordocl datadtrtll used In DOSDDS analysisan~lysis New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 r~"""""'6!- Conference on Applied Statistics in Agriculture L ~a \ ...,....--1 ------Kansas State University FigureFigure 2.2. Green'sGreen's FunctionFunction "' I CyclicCyclic ThermalThermal StressStress II! ARIMAARIMA (4,24,3)(4,24,3) SteerSteer 219219 I! COMPOSIT[COMF'OSITE 1 o· 0.90.9 G.B'O.fl \).7'().7 . cC o0 \).6-0.6- Mt1 PP 0.S· o0 S 05 s n.11."· 'I· II T 1 T 0.3 E o 2 ',.'~ 0.1 0.0· *'+ .. 4-'" .;.--~ .. k"'''",._ . - ···----...... F+ ~t' ._.~ ~o.-0. !1 - ,"--.------ro--,---.----,--,---,.-'-r,---,---' --r-,--, '""-r--'-T-'--. --'--'---.-----.--r-T'-~....,~--'--,.------r-r-.,.--' 'T-'-'- ,-'.-' . ...-r ,. ,...·r-.,.~-r (J I"IU :'U~~() :-IU -II) GU " ~H1 -II) !.;o TIt1ErIME 78;( COMPLEX CONJUGATE 7eA COMPLEX CONJUGATE 22X22X COMPLEXCOMPLEX CONJUGATE GI CONJUGATE GI I. G G2G2 I. G' 0.3-0.3 0.9 O.g· 0.g· \).8' 0.7· 0.2fJ.2~ I) 0- I) S O.0.1 I Il'] '~ 1 (3 I ~..... ~-",,* .....~. I 3 .~'''-*, r""-* ,/1<"""'" o (l.j ~---~-/'y,)' '*" ,r~,r,,' . /'" .. ! \) 2 (). G -....~ ----~7----7- --·------'~-7--,\---7"'--- New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 r------.--- Conference on Applied Statistics in Agriculturel' Figure 3. Phase Diagrarrls Kansas State Universityr' for Tympanic Temperature CYCLIC THERMONEUTRAL STEER 185 CYCIJCCYCLIC TI-IJi:HMALTI-mHMAL STHESS s-rCER 106 Xx 39.8-39.(\' x " "I ~C0 ~~)\ .-----:<;;c~~~:) .1 t--.'f'I'1 1/1//1 4 ~ /I~II ·10 ~)- .~/ /d 38.0' ·1· + ~,~f5~~ 39.5-:=It), s- y+ + .~/y +& ,. Ih=d:;:r?-~ + + --l~·+-----:r· ' 37 . !) 'l,-~:r~"------""":!~~'--~"T---'------~'------""'------'---'------"-----'------'------1------'-----'-----'------1-----;- 3 (3 5 ~I.-----...... :,.~ __ ,---.----y ---.---.-.--T.---,------.,-.-.~ , _-,----,---.,-___ ,"_ 37.837.13 38.8 39.8 ~W. 5 39.S ~O.540.5 -441 \ . S Y s CONSTANT THERMONEUTRi\LTHERMONEUTRAL CONSTANTCON~';TANT THERMAL STRESS STEER 179 d. STEER 179 xX x 39.8' '\.j \ ..5- S + + + + -10.5'10.5 - + ~~.=+o ~+ -bit+. i'Y++ + 38.038.8 3D s- 37. 0 l1-----T----.,---!-~,...... ,_.,.-___,----,-..._____r_-,-~--,.----,---,--- J8 S "if ---'--...,.--I-,--'------,-----r--I- 31.637.(3 38.038.S 39 II 38.5 JCJ.S 40.5 41 . s y y I I ,------.-.------~------.--~~ New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4 -.---~----.-~--~-~~--~~------.------.------.--~----.------_. Conference on Applied Statistics in Agriculture r------Figure 4. Spectral Analysis ------lKansas State University for Tympanic Temperature CYCLIC THERMONEUTHALTHE~RMONEUTHAL SPECTRAL ANALYSIS CYCLIC THERMALTIIE:RMAL STRESS STEERSTETR 186 SPECTRAL ANALYSIS STEER 188185 o 28 ~ ~ 0 26 sS 11 4 i E 0 21·j f' 1 E 1 ~ C. 22 -~ C~ R 0.201 1 3 A ~R 3 LB. 18 i A L G If!1(3 D0 0 EO.E \) 14·1'1- D N F 2 S B.0 12 N S I 0 10·I\)- 1 I Y () OilOfl Tr Yy (lo 0 DOuo- o I·1- 0G. 01·04 - r· X B.02·0.02- x 0000.00 .. ------rl------. --r----~------~ () ·1,-~~--====--.- ,=-~. ______-,-______,-----__._._--. T ~~ A~~_AA'~A----.------1 ------·----T----T : 0 t=---~-· ~'-,- 0 234;~ 3 4 o 2 3 4 FREOW'NCYFr~F.(JUFNCY FROM 130 TO PI1'1 FREQUENCYFREOUENCY FROM 0B TO PI CONSTANT THERMOTHERMONEUTRAL NEUTRAL CONSTANT THERMAL STRESS SPECTRAL ANALYSIS SPECTRAL ANALYSIS STEER 179 STEER 171l17[J oG.07 07 0.9 sS pP Ss 0 g~1-1 [E 0.06·0.06 Pp 0.8 C E T C o -, R O.OS0.05 ~T 0.7.1 A R L A 0.6C.G L D B. 0 B-1CH - L I E D 0.5G.S N E ~S B.03 0 G3 N~ 13_4-0.4 II S T 1 I Yy Bil. B2n2 I T 0.30_3 Y o0 0.2(J.2 FI' 0.01·G 01 - o0 F X O.0.1 I X 0.00·0.00 I .~ 0.0(J.0 r··----· T ,------_.,------, r------T B I 2 3 4 0230 I 4 w l FREOUENCYFREQUENCY FROM 013 10TO PI FREQUENCYfREQUENCY FROMfROM 0 TO PI w New Prairie Press https://newprairiepress.org/agstatconference/1989/proceedings/4