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  • 1
    ISSN: 0095-9898
    Keywords: Life and Medical Sciences ; Cell & Developmental Biology
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Biology , Medicine
    Notes: Non-torpid P. californicus have body temperatures which increase slightly as ambient temperature increases from 5° to 35°C. Their minimum oxygen consumption fits Newton's law of cooling, since minimum thermal conductance below thermal neutrality is virtually constant at 0.19 ml O2 (gm hr °C)-1. There is a thermal neutral point at 32.5° rather than a thermal neutral zone. Oxygen consumption at the thermal neutral point is 0.97 ml O2 (gm hr)-1. Maximum thermal conductance, measured at 35°, is 0.37 ml O2 (gm hr °C)-1. Evaporative water loss accounts for 5 and 15% of the value of minimum and maximum thermal conductance, respectively.Minimum oxygen consumption of mice in torpor is continuously dependent on body temperature from thermal neutrality to deep torpor. Q10 values are between 1.6 and 3.2. The thermal conductance of torpid mice at ambient temperature below 30° is 0.19 ml O2 (gm hr °C)-1 which is identical to the minimum thermal conductance of non-torpid mice. Torpid mice at an ambient temperature of 30° have thermal conductance values between 0.23 and 0.40 ml O2 (gm hr °C)-1 depending on their posture.Maximum oxygen consumption is linearly related to body temperature. At a normal body temperature of 38°, it is 11.6 ml O2 (gm hr)-1 which is no greater than that of similar sized mammals which do not enter torpor.Although P. californicus consistently enters into and arouses from torpor at ambient temperatures of 15° to 30°, the torpor cycle is severely disturbed at temperatures between 10° and 12°. At these temperatures mice show irregular temporal patterns of torpor, do not enter torpor completely, and cannot arouse from torpor if body temperature falls below 15°.Observations on the behavior of torpid and non-torpid P. californicus at various ambient temperatures are included in this report.
    Additional Material: 6 Ill.
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  • 2
    ISSN: 0095-9898
    Keywords: Life and Medical Sciences ; Cell & Developmental Biology
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Biology , Medicine
    Notes: The changes in body temperature (TB) associated with the torpor cycle of P. californicus are described by the equation \documentclass{article}\pagestyle{empty}\begin{document}$ \frac{{{\rm dT}_{\rm B} }}{{{\rm dt}}} = \frac{{{\rm heat production - heat loss}}}{{\rm K}} $\end{document} where t is time, and K is the heat capacity of body tissue. This equation can be solved after substituting appropriate expressions for maximum and minimum aerobic heat production and heat loss to give theoretical maximum rates of entry into and arousal from torpor.The measured time course of body temperature and oxygen consumption during entry into torpor compare favorably with theoretical curves calculated under conditions of minimum heat production and maximum heat loss. Thus P. californicus appears able to “switch off its thermostat” so that oxygen consumption during entry into torpor falls almost to the minimum level for a given body temperature. Heat loss during entry into torpor appears to be facilitated by an increase in thermal conductance.During arousal from torpor, body temperature increases faster than can be accounted for assuming maximum heat production and minimum heat loss. This could be explained by anaerobic heat production and by a decreased thermal conductance resulting from the posterior vasoconstriction typical of arousing hibernators.Torpor periods of short duration are feasible for P. californicus, for it can enter torpor and arouse immediately thereafter at an ambient temperature of 15° with an expenditure of energy only 55% of that required to maintain a high body temperature over the same period of time. Arousal from torpor at an ambient temperature of 15° requires about 75% of the total energy expended during a ten hour torpor cycle; entry into torpor and torpor itself account for only 9 and 16% of the total energy expenditure, respectively.The quantitative relations between heat production and heat loss presented in this paper suggest further investigations of the effects of body size on heat production and loss, and of physiological phenomena which alter heat exchange.
    Additional Material: 5 Ill.
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