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Modern Engineering Thermodynamics

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710 CHAPTER 17: <strong>Thermodynamics</strong> of Biological Systems<br />

IS IT A Calorie OR A calorie?<br />

When the word calorie is capitalized, it indicates what nutritionalists call a large calorie, or a kilocalorie. That is, in nutrition<br />

jargon, 1 Calorie = 1 kilocalorie, yet it takes 1000 calories to equal 1 kilocalorie. Only the capital C distinguishes the two.<br />

So, when a nutrition table indicates that your caloric intake should be 2500 Calories per day, it really means 2500 kilocalories<br />

per day. Now, since 1 kilocalorie = 4.186 kilojoules, then 2500 Calories/d = 2500 kcal/d = (2500 kcal/d)(4.186 kJ/<br />

kcal) = 10,465 kJ/d = 10.456 MJ/d.<br />

From Table 17.5, we find that the energy expenditure required to jog, play football, or fast dance is about 600 Calories per<br />

hour, and Table 17.4 tells us that the energy content of milk chocolate is about 150 Calories per ounce. So, if you want to<br />

exercise off the energy content of one 1.5-oz milk chocolate candy bar you would have to jog, play football, or fast dance<br />

continuously for<br />

This is a lot of hard exercise for one small candy bar.<br />

ð1:5ozÞð150 Calories/ozÞ<br />

600 Calories/h<br />

= 0:375 hours<br />

EXAMPLE 17.6<br />

Suppose you want to exercise off the energy added to your body as a result of eating one pint of ice cream by lifting<br />

weights. The external work done by the body equals the change in potential energy of the weights as they are lifted (there is<br />

no significant energy recovery within the body, however, when the weights are lowered again). Suppose you are lifting 490.<br />

N (110. lbm) a vertical distance of 1.00 m, and you can make one lift in 1.00 second. Approximately how many lifts are<br />

required and how long will it take to work off the energy content of the ice cream?<br />

Solution<br />

Each lift requires that an amount of energy be put into the weights of<br />

ðmgZ/g c<br />

Þ weights<br />

= ð490: NÞð1:00 mÞ/1<br />

ð Þ = 490: N.m = 490: J<br />

If we take the human body as the thermodynamic system and apply the energy rate balance and ignore all mass flow energy<br />

movements into or out of the system during the exercise period (thus, we are ignoring perspiration energy losses and all O 2<br />

and CO 2 exchanges), then we can write<br />

<br />

_Q − _W =<br />

dU + d <br />

mV 2<br />

+ d <br />

mgZ<br />

dt dt 2g c dt g c<br />

Since the kinetic and potential energies of the human body do not change significantly during the exercise, we can set<br />

and the energy rate balance becomes<br />

<br />

d mV 2<br />

dt 2g c<br />

+ d dt<br />

<br />

_Q − _W =<br />

dU <br />

dt<br />

Now, the external work rate that must be done by the system is<br />

<br />

mgZ<br />

g c<br />

body<br />

<br />

body<br />

= _U body<br />

= 0<br />

body<br />

ð<br />

_W = − mgZ/g cÞ weights<br />

= 490: J = 490: J=s<br />

Δt 1:00s<br />

It has been shown experimentally that the energy conversion efficiency of animal muscular contraction defined by<br />

Eq. (17.12) is about 25%, or<br />

ðη T Þ muscle<br />

=<br />

_W<br />

_U body<br />

= 0:250

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