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A power plant produces1GWof electricity, at an efficiency of 40%(typical of today's coal-fired plants).

(a) At what rate does this plant expel waste heat into its environment?

(b) Assume first that the cold reservoir for this plant is a river whose flow rate is 100m3/s.By how much will the temperature of the river increase?

(c) To avoid this "thermal pollution" of the river, the plant could instead be cooled by evaporation of river water. (This is more expensive, but in some areas it is environmentally preferable.) At what rate must the water evaporate? What fraction of the river must be evaporated?

Short Answer

Expert verified

a) Rate of heat expel is 1.5GW

b) Change in temperature of river water is 3.5k

c) Water evaporate at rate663.7kg/s

Step by step solution

01

Part (a) - Step 1: To determine

The rate at which this plant expel waste heat into environment

02

Part (a) - Step 2: Explanation

Given:

Power output:P=1GW

Efficiency of plant,e=40%=0.4

Formula for efficiency heat engine is :

e=WQh=WQc+W

Here

W : is the work done

Qh: is the heat extract from hot reservoir and

Qcis the heat expel into cold reservoir.

We know efficiency of heat engine =WQh

Also we have the formulaW=Qh-QCOrQh=W+QC

So we have efficiency,e=WW+Qc

From this we haveQc=W1e-1

In the given:

Efficiency,e=40%=0.4

We know power P=WtOrW=P×t

Here t=1sandP=109W

So work done in one second is W=109J

So heat goes into environment in one second is Qc=W1e-1

Now substitute the values

Qc=10910.4-1=1.5×109J

Hence Rate at which heat is expel into environment is1.5GW

03

Part (b) - Step 3: To find

By how much will the temperature of river increase.

04

Part (b) - Step 3: Explanation

Given :

River flow rate, VË™=100m3/sec

Heat expel in the river in one second,Qc=1.5×109J

Specific heat of water, s=4186JkgK

Heat transfer,Qc=msΔT

Where,

sis the specific heat,

mis mass

Calculation:

Qc=msΔT

And , ÒÏ=mV

Here ÒÏis density of water,

mis the mass and V in volume.

We know density of water,ÒÏ=1000kg/m3

Since volume of water flow in one second isV=100m3

So mass of water flow in one second ism=ÒÏV=105kg

Heat transfer, Qc=msΔT

Then

ΔT=Qc(m)(s)=1.5×109105×4186JkgKRK=3.5K

Hence change in temperature of river water 3.5k

05

Part (c) - Step 5: To find

The rate at which the water evaporate

06

Part (c) - Step 6: Explanation

Given:

River flow rate, VË™=100m3/sec

Heat expel in the river in one second, Qc=1.5×109J

Latent heat of evaporation of water, LV=2260×103Jkg

Formula used:

Heat transfer during evaporation, QVap=mLV

Calculation:

Heat transfer during evaporation, QVap=mLV

All of the expelled heat is converted to evaporation heat.

So,QVap=Qc=1.5×109J

Mass of water evaporate in one second, m=1.5×109J2260×103Jk=663.7kg/s

Hence rate at which water evaporate is663.7kg/s

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Most popular questions from this chapter

An apparent limit on the temperature achievable by laser cooling is reached when an atom's recoil energy from absorbing or emitting a single photon is comparable to its total kinetic energy. Make a rough estimate of this limiting temperature for rubidium atoms that are cooled using laser light with a wavelength of 780 nm.

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Prove that if you had a heat engine whose efficiency was better than the ideal value (4.5), you could hook it up to an ordinary Carnot refrigerator to make a refrigerator that requires no work input.

At a power plant that produces 1 GW109 watts) of electricity, the steam turbines take in steam at a temperature of 500o, and the waste heat is expelled into the environment at 20o
(a) What is the maximum possible efficiency of this plant?
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The ingenious Stirling engine is a true heat engine that absorbs heat from an external source. The working substance can be air or any other gas. The engine consists of two cylinders with pistons, one in thermal contact with each reservoir (see Figure 4.7). The pistons are connected to a crankshaft in a complicated way that we'll ignore and let the engineers worry about. Between the two cylinders is a passageway where the gas flows past a regenerator: a temporary heat reservoir, typically made of wire mesh, whose temperature varies

gradually from the hot side to the cold side. The heat capacity of the regenerator is very large, so its temperature is affected very little by the gas flowing past. The four steps of the engine's (idealized) cycle are as follows:
i. Power stroke. While in the hot cylinder at temperature Th, the gas absorbs heat and expands isothermally, pushing the hot piston outward. The piston in the cold cylinder remains at rest, all the way inward as shown in the figure.
ii. Transfer to the cold cylinder. The hot piston moves in while the cold piston moves out, transferring the gas to the cold cylinder at constant volume. While on its way, the gas flows past the regenerator, giving up heat and cooling to Tc.
iii. Compression stroke. The cold piston moves in, isothermally compressing the gas back to its original volume as the gas gives up heat to the cold reservoir. The hot piston remains at rest, all the way in.
iv. Transfer to hot cylinder. The cold piston moves the rest of the way in while the hot piston moves out, transferring the gas back to the hot cylinder at constant volume. While on its way, the gas flows past the regenerator, absorbing heat until it is again at Th.

(a) Draw a PV diagram for this idealized Stirling cycle.
(b) Forget about the regenerator for the moment. Then, during step 2, the gas will give up heat to the cold reservoir instead of to the regenerator; during step 4 , the gas will absorb heat from the hot reservoir. Calculate the efficiency of the engine in this case, assuming that the gas is ideal. Express your answer in terms of the temperature ratio Tc / Th and the compression ratio (the ratio of the maximum and minimum volumes). Show that the efficiency is less than that of a Carnot engine operating between the same temperatures. Work out a numerical example.
(c) Now put the regenerator back. Argue that, if it works perfectly, the efficiency of a Stirling engine is the same as that of a Carnot engine.
(d) Discuss, in some detail, the various advantages and disadvantages of a Stirling engine, compared to other engines.

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