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Modern Engineering Thermodynamics

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17.9 <strong>Thermodynamics</strong> of Aging and Death 717<br />

Table 17.6 Metabolic Characteristics of Typical Mammals<br />

Mammal<br />

Body Mass (kg)<br />

Pulse Rate<br />

(beats/min)<br />

Breathing Rate<br />

(breaths/min)<br />

Life Span (years)<br />

Shrew 0.003 1030 230 3.7<br />

Mouse 0.03 580 130 5.9<br />

Rat 0.2 360 80 8.6<br />

Cat 2.8 190 42 14<br />

Dog 15.9 120 27 21<br />

Horse 700 47 10 44<br />

Elephant 4000 30 6.7 62<br />

Even though we know that the metabolic heat generation rate _Q decreases with increasing age (e.g., see<br />

Figure 17.6), this effect must be offset by increasing size (i.e., growth) and eating less or exercising less as age<br />

increases. Experiments in which test animals were fed a very low (starvation level) daily diet showed that<br />

they generally had a lower metabolic rate and lived longer than did their counterparts who were fed a normal<br />

or excessive diet. These particular results, however, occur only when the starvation diet was begun before the<br />

animal reached sexual maturity. If it was begun later in life, it had no significant effect on metabolic rate or on<br />

life span.<br />

An entropy rate balance on a living system is<br />

_Q<br />

+∑ _ms −∑ _ms + _S P = dS<br />

T b in out<br />

dt<br />

(17.27)<br />

The first term is the entropy transport due to the metabolic heat transfer, and since _Q < 0, it is negative. The<br />

combination of the second and third terms is the net entropy transport into the system via the mass flow<br />

of food, respiration, and wastes. Since the entropy of the incoming food is lower than the entropy of the<br />

outgoing wastes (both are at the same temperature, but the molecular order of the food is more complex<br />

than that of the wastes) and the input and output mass flow rates averaged over a long period of time are<br />

essentially the same, these two terms taken together also are negative. The last term on the left side of<br />

Eq. (17.27) is the rate of entropy production, which by the second law of thermodynamics must always be<br />

positive. The term on the right side is the time rate of changeoftheentropyoftheentirebiologicalsystem,<br />

and it can be either positive or negative depending on the net sign of the left side. Thus, we find that, for<br />

any living system,<br />

_S P > 0<br />

_Q<br />

T b<br />

< 0<br />

∑<br />

in<br />

_ms −∑<br />

out<br />

_ms < 0<br />

But, these conditions alone are not sufficient to define a living system. The one characteristic that seems to make<br />

a living system unique is its peculiar affinity for self-organization, and this characteristic corresponds to a continual<br />

decrease in the system’s entropy over its life span. As the system “lives,” it grows and ages and generally<br />

CRITICAL THINKING<br />

Is life unique in your opinion? That is, are living systems scientifically distinguishable from nonliving systems? Given a<br />

sealed box containing an object, how can you tell whether or not the object is living without opening the box? What physical<br />

tests could you perform to determine the life state of the object in the box?

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