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How much work must be done by a Carnot refrigerator to transfer 1.0 J as heat (a) from a reservoir at 7.0°Cto one at 27°C, (b) from a reservoir at -73°Cto one at 27°C, (c) from a reservoir at -173°Cto one at 27°C, and (d) from a reservoir at -233°Cto one at 27°C?

Short Answer

Expert verified
  1. The work done by the Carnot refrigerator from a reservoir at 7°Cto one at 27°Cis 0.071J
  2. The work done by the Carnot refrigerator from a reservoir at-73°Cto one at 27°Cis 0.50J.
  3. The work done by the Carnot refrigerator from a reservoir at to one at -173°Cto one at 27°Cis 2.0J.
  4. The work done by the Carnot refrigerator from a reservoir at to one at-233°Cto one at 27°Cis 5.0J.

Step by step solution

01

The given data

Energy transferred by the Carnot refrigerator as heat,QL=1.0J

02

Understanding the concept of the Carnot refrigerator

A Carnot refrigerator operates as a reversible Carnot cycle by rejecting the heat of the freezer to the environment. Thus, using the work done and its performance relation, we can get the required work values in each given case.

Formulae:

The coefficient of performance of a Carnot refrigerator,KC=TLTH-TL (1)

The work done per cycle of a Carnot refrigerator, W=QLKc (2)

03

a) Calculation of the work done from 7oC to 27oC

Here, the low temperature of the reservoir is at TL=7°C=280Kand the high temperature is at TH=27°C=300K

Now, the work done by the Carnot refrigerator from a reservoir at 7°Ctooneat27°Cis given by substituting equation (1) in equation (ii) with the given data as follows:

W=QLTH-TLTL=(1.0J)300K-280K280K=0.071J

Hence, the value of the work done is 0.071J.

04

b) Calculation of the work done from -73oC to 27oC

Here, the low temperature of the reservoir is atTL=-73°C=200Kand the high temperature is atTH=27°C=300K

Now, the work done by the Carnot refrigerator from a reservoir at-73°Cto one at27°Cis given by substituting equation (1) in equation (2) with the given data as follows:

W=QLTH-TLTL=(1.0J)300K-200K200K=0.50J

Hence, the value of the work done is 0.50 J.

05

c) Calculation of the work done from -173oC to 27oC

Here, the low temperature of the reservoir is atTL=-173°C=100Kand the high temperature is atTH=27°C=300K

Now, the work done by the Carnot refrigerator from a reservoir at173°Cto one at27°Cis given by substituting equation (1) in equation (2) with the given data as follows:

W=QLTH-TLTL=(1.0J)300K-100K100K=2.0J

Hence, the value of the work done is 2.0 J.

06

d) Calculation of the work done from -223oC to 27oC

Here, the low temperature of the reservoir is atTL=-223°C=50Kand the high temperature is atTH=27°C=300K

Now, the work done by the Carnot refrigerator from a reservoir at-233°Cto one at27°Cis given by substituting equation (1) in equation (2) with the given data as follows:

W=QLTH-TLTL=(1.0J)300K-50K50K=5.0J

Hence, the value of the work done is 5.0 J.

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Most popular questions from this chapter

Suppose 1.0 molof a monatomic ideal gas initially at 10 Land 300 K is heated at constant volume to 600 K, allowed to expand isothermally to its initial pressure, and finally compressed at constant pressure to its original volume, pressure, and temperature. During the cycle, what are (a) the net energy entering the system (the gas) as heat and (b) the net work done by the gas? (c) What is the efficiency of the cycle?

A box contains gas molecules. Consider the box to be divided into three equal parts. (a) By extension of Eq. 20-20, write a formula for the multiplicity of any given configuration. (b) Consider two configurations: configuration Awith equal numbers of molecules in all three thirds of the box, and configuration B with equal numbers of molecules in each half of the box divided into two equal parts rather than three. What is the ratio WA/WB of the multiplicity of configuration A to that of configuration B ? (c) EvaluateWA/WBfor N = 100. (Because is not evenly divisible by 3, put 34 molecules into one of the three box parts of configuration Aand 33 in each of the other two parts.)

A three-step cycle is undergone by 3.4mol of an ideal diatomic gas: (1) the temperature of the gas is increased from 200 K to 500 Kat constant volume; (2) the gas is then isothermally expanded to its original pressure; (3) the gas is then contracted at constant pressure back to its original volume. Throughout the cycle, the molecules rotate but do not oscillate. What is the efficiency of the cycle?

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(a) A Carnot engine operates between a hot reservoir at 320 Kand a cold one at 260 K. If the engine absorbs 500 Jas heat per cycle at the hot reservoir, how much work per cycle does it deliver? (b) If the engine working in reverses functions as a refrigerator between the same two reservoirs, how much work per cycle must be supplied to remove 1000Jas heat from the cold reservoir?

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