Chapter 6: Problem 13
What would the maximum thermodynamic efficiency be of some heat engine operating between your skin temperature and the ambient environment \(20^{\circ} \mathrm{C}\) cooler than your skin?
Chapter 6: Problem 13
What would the maximum thermodynamic efficiency be of some heat engine operating between your skin temperature and the ambient environment \(20^{\circ} \mathrm{C}\) cooler than your skin?
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In a house achieving a heat loss rate of \(200 \mathrm{~W} /{ }^{\circ} \mathrm{C}\) equipped a \(5,000 \mathrm{~W}\) heater, what will the internal temperature be if the outside temperature is \(-10^{\circ} \mathrm{C}\) and the heater is running \(100 \%\) of the time?
How many Joules does it take to heat your body up by \(1^{\circ} \mathrm{C}\) if your (water-dominated) mass has a specific heat capacity of \(3,500 \mathrm{~J} / \mathrm{kg} /{ }^{\circ} \mathrm{C} ?\)
Since the sun drives energy processes on Earth, we could explore the maximum possible thermodynamic efficiency of a process operating between the surface temperature of the sun \((5,800 \mathrm{~K})\) and Earth's surface temperature \((288 \mathrm{~K}) .\) What is this maximum efficiency? \(^{69}\)
If a can of soda \(\left(350 \mathrm{~mL} ;\right.\) treat as water) cools from \(20^{\circ} \mathrm{C}\) to \(0^{\circ} \mathrm{C}\), how much energy is extracted, and how much is the entropy (in \(\mathrm{J} / \mathrm{K}\) ) in the can reduced using the average temperature and the relation that \(\Delta Q=T \Delta S ?\)
We can think of wind in the atmosphere as a giant heat engine \(^{67}\) operating between the \(288 \mathrm{~K}\) surface and the top of the troposphere \(^{68}\) at \(230 \mathrm{~K}\). What is the maximum efficiency this heat engine could achieve in converting solar heating into airflow?
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