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1
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0000664818
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Body size and metabolism
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M. Kleiber, "Body size and metabolism," Hilgardia 6, 315-353 (1932); M. Kleiber, The Fire of Life (Wiley, New York, 1961).
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(1932)
Hilgardia
, vol.6
, pp. 315-353
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Kleiber, M.1
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2
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0004222696
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Wiley, New York
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M. Kleiber, "Body size and metabolism," Hilgardia 6, 315-353 (1932); M. Kleiber, The Fire of Life (Wiley, New York, 1961).
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(1961)
The Fire of Life
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Kleiber, M.1
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4
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0038307949
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Wiley, New York, 2nd ed.
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goose down =0.025 by J. D. Cutnell and K. W. Johnson, Physics (Wiley, New York, 1992), 2nd ed., p. 366. Deep diving animals cannot use an air layer trapped in fur or feathers as insulation since gas is compressible, so that the thickness ΔR and hence the thermal resistance s =ΔR/k would decrease with depth.
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(1992)
Physics
, pp. 366
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Cutnell, J.D.1
Johnson, K.W.2
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5
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0019978393
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Energy metabolism and body size. I. Is the 0.75 mass exponent of Kleiber's equation a statistical artifact?
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A. A. Heusner, "Energy metabolism and body size. I. Is the 0.75 mass exponent of Kleiber's equation a statistical artifact?" Respir. Physiol. 48, 1-12 (1982).
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(1982)
Respir. Physiol.
, vol.48
, pp. 1-12
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Heusner, A.A.1
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6
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0020593906
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The 3/4 mass exponent for energy metabolism is not a statistical artifact
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H. A. Feldman and T. A. McMahon, "The 3/4 mass exponent for energy metabolism is not a statistical artifact," Respir. Physiol. 52, 149-163 (1983).
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(1983)
Respir. Physiol.
, vol.52
, pp. 149-163
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Feldman, H.A.1
McMahon, T.A.2
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7
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85033950087
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See Ref. 2, p. 61
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See Ref. 2, p. 61.
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9
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0004227496
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Scientific American Library, distributed by Freeman, New York
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T. A. MacMahon and J. T. Bonner, On Size and Life (Scientific American Library, distributed by Freeman, New York, 1983), p. 255.
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(1983)
On Size and Life
, pp. 255
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MacMahon, T.A.1
Bonner, J.T.2
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10
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85033956588
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note
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2.
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11
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85033954939
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note
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i + 2R). However, it was noted that the heat losses through the cylindrical wall and the end caps were equal within a few percent to the heat losses of a cylinder of radius R and length L that conducts heat only through its cylindrical wall. Therefore, we approximated aquatic mammals as cylinders of length L with no thermal end losses.
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13
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85033957359
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See Ref. 2, p. 198
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See Ref. 2, p. 198.
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