(a) During each cycle, a Carnot engine absorbs 750 Jas heat from a high-temperature reservoir at 360 K , with the low-temperature reservoir at 280 K . How much work is done per cycle? (b) The engine is then made to work in reverse to function as a Carnot refrigerator between those same two reservoirs. During each cycle, how much work is required to remove 1200Jas heat from the low-temperature reservoir?

Short Answer

Expert verified
  1. Work done per cycle of Carnot engine is 166.5 J
  2. Work required to remove 1200 J as heat from the low-temperature reservoir is 342.8 J

Step by step solution

01

 Step 1: The given data

The high-temperature reservoir is at,TH=360K

The low-temperature reservoir is at,TL=280K

Heat absorbed from the high-temperature reservoir isQH=750J

Heat absorbed from the low-temperature reservoir is QL=1200J

02

Understanding the concept of the Carnot engine

Using the equations for the efficiency of the Carnot engine, we can find the work done per cycle. We can find the work required to remove heat using the formulae for the coefficient of performance of the refrigerator.

Formulae:

The efficiency of the engine,

ε=WQH (1)

The efficiency of the Carnot cycle,

ε=1-QLQH=1-TLTH (2)

Coefficient of performance of refrigerator,

K=QLW (3)

Coefficient of performance for Carnot cycle,

Kc=QLQH-QL=TLTH-TL (4)

03

(a) Calculation of work done per cycle of Carnot engine

From the equation (2) of efficiency of the Carnot cycle, we can get that

εc=1-280K360K=0.222

Substituting the given values in equation (1), we can get the work done per cycle of the engine is given as:

0.222=W750W=166.5J

Hence, the work done per cycle of the engine is 166.5 J

04

(b) Calculation of required work to remove as heat from the low-temperature reservoir

The coefficient of performance Kcfor the Carnot cycle using equation (4) is given by:

Kc=280K360K-280K=3.5

Since the Carnot engine is made to work as a refrigerator

So, the coefficient of performance K of the refrigerator using equation (3) is given as:

3.5=1200WW=342.8J

Hence, the work done per cycle of the refrigerator is 342.8 J

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Most popular questions from this chapter

An inventor claims to have invented four engines, each of which operates between constant-temperature reservoirs at 400 and 300K. Data on each engine, per cycle of operation, are: engine A, QH=200J,QL=175J, and W = 40 J; engine B, QH=500J,QL=-200J,and W = 400 J; engine C, QH=600J,QL=-200J, and W = 400 J; engine D,QH=100J,QL=-90J, and W = 10J. Of the first and second laws of thermodynamics, which (if either) does each engine violate?

Figure 20-36 shows a Carnot cycle on a T-Sdiagram, with a scale set bySs=0.60J/K. For a full cycle, find (a) the net heat transfer and (b) the net work done by the system.

The temperature of 1.00 mol of a monatomic ideal gas is raised reversibly from 300 K to 400 K , with its volume kept constant. What is the entropy change of the gas?

Suppose that a deep shaft were drilled in Earth’s crust near one of the poles, where the surface temperature is -40oC , to a depth where the temperature is 800°C. (a) What is the theoretical limit to the efficiency of an engine operating between these temperatures? (b) If all the energy released as heat into the low-temperature reservoir were used to melt ice that was initially at -40oC , at what rate could liquid water at 0°C be produced by a 100 MW power plant (treat it as an engine)? The specific heat of ice is 2220J/kg·K; water’s heat of fusion is 333J/kg·K. (Note that the engine can operate only between and in this case. Energy exhausted at-40°Ccannot warm anything above-40°C .)

Figure 20-32 represents a Carnot engine that works between temperatures T1=400K andT2=150K and drives a Carnot refrigerator that works between temperatures T3=325KandT4=225K . What is the ratioQ3/Q1 ?

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