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Question: Suppose a heat pump has a stationary bicycle attachment that allows you to provide the work instead of using an electrical wall outlet. If your heat pump has a coefficient of performance of 2.0 and you can cycle at a racing pace (Table 15–2) for a half hour, how much heat can you provide?

Short Answer

Expert verified

The heat delivered to the heat pump is \(4.572 \times {10^6}\;{\rm{J}}\).

Step by step solution

01

Determination of the coefficient of performance

The coefficient of performance of a heat pump can be calculated by dividing the heat intake by the pump by the work performed by the pump.

02

Given information

The coefficient of performance of the pump is \({\rm{COP}} = {\rm{2}}{\rm{.0}}\).

03

Evaluation of the work input to the heat pump

From table 15-2, the metabolic rate for bicycling is \(1270\;{{\rm{J}} \mathord{\left/{\vphantom {{\rm{J}} {\rm{s}}}} \right.} {\rm{s}}}\).

The work input to the heat pump is calculated below:

\(\begin{aligned}{l}W &= \left( {1270\;{{\rm{J}} \mathord{\left/{\vphantom {{\rm{J}} {\rm{s}}}} \right.} {\rm{s}}}} \right)\left( {0.5\;{\rm{h}}} \right)\left( {\frac{{3600\;{\rm{s}}}}{{1\;{\rm{h}}}}} \right)\\W &= 2.286 \times {10^6}\;{\rm{J}}\end{aligned}\)

04

Evaluation of the heat delivered to the heat pump

The heat delivered to the heat pump is calculated below:

\(\begin{aligned}{l}{Q_{\rm{H}}} &= W\left( {{\rm{COP}}} \right)\\{Q_{\rm{H}}} &= \left( {2.286 \times {{10}^6}\;{\rm{J}}} \right)\left( {2.0} \right)\\{Q_{\rm{H}}} &= 4.572 \times {10^6}\;{\rm{J}}\end{aligned}\)

Thus, the heat delivered to the heat pump is \(4.572 \times {10^6}\;{\rm{J}}\).

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Most popular questions from this chapter

Question: (III) The PV diagram in Fig. 15–23 shows two possible states of a system containing 1.75 moles of a monatomic ideal gas. \(\left( {{P_1} = {P_2} = {\bf{425}}\;{{\bf{N}} \mathord{\left/{\vphantom {{\bf{N}} {{{\bf{m}}^{\bf{2}}}}}} \right.} {{{\bf{m}}^{\bf{2}}}}},\;{V_1} = {\bf{2}}{\bf{.00}}\;{{\bf{m}}^{\bf{3}}},\;{V_2} = {\bf{8}}{\bf{.00}}\;{{\bf{m}}^{\bf{3}}}.} \right)\) (a) Draw the process which depicts an isobaric expansion from state 1 to state 2, and label this process A. (b) Find the work done by the gas and the change in internal energy of the gas in process A. (c) Draw the two-step process which depicts an isothermal expansion from state 1 to the volume \({V_2}\), followed by an isovolumetric increase in temperature to state 2, and label this process B. (d) Find the change in internal energy of the gas for the two-step process B.

(II) Water is stored in an artificial lake created by a dam (Fig. 15–27). The water depth is 48 m at the dam, and a steady flow rate of\({\bf{32}}\;{{\bf{m}}{\bf{3}}}{\bf{/s}}\)is maintained through hydroelectric turbines installed near the base of the dam. How much electrical power can be produced?

FIGURE 15-27 Problem 55

The oceans contain a tremendous amount of thermal (internal) energy. Why, in general, is it not possible to put this energy to useful work?

An ideal gas undergoes an adiabatic expansion, a process in which no heat flows into or out of the gas. As a result,

(a) the temperature of the gas remains constant and the pressure decreases.

(b) both the temperature and pressure of the gas decrease.

(c) the temperature of the gas decreases and the pressure increases.

(d) both the temperature and volume of the gas increase.

(e) both the temperature and pressure of the gas increase

Calculate the work done by an ideal gas while going from state A to state C in Fig. 15–28 for each of the following processes:

(a) ADC,

(b) ABC, and

(c) AC directly.

FIGURE 15–28

Problem 68

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