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When the sun is high in the sky, it delivers approximately 1000 watts of power to each square meter of earth's surface. The temperature of the surface of the sun is about 6000K, while that of the earth is about 300K.

(a) Estimate the entropy created in one year by the flow of solar heat onto a square meter of the earth.

(b) Suppose you plant grass on this square meter of earth. Some people might argue that the growth of the grass (or of any other living thing) violates the second law of thermodynamics, because disorderly nutrients are converted into an orderly life form. How would you respond?

Short Answer

Expert verified

(a) The change in entropy can be estimated to be 4.97×107JK-1.

(b) The growth of grass doesn't violate the second law of thermodynamics as the entropy produced to transmit the energy from the sun to earth (disordered) would be much higher when compared to the entropy produced by the biochemical reactions (ordered) in the grass.

Step by step solution

01

Part (a) Step 1: Given

Power delivered per square meter=Ps=1000W

Surface temperature of sun =Tsun=6000K

Surface temperature of earth Tearth=300K

Time period (day time)role="math" localid="1647243842287" =t=1year=12×3600×365s

02

Part (a) Step 2: Calculation

Amount of energy received by the earth per square meter can be calculated as:

Q=Ps×t

By substituting the values, we get,

Q=1000×(12×3600×365)Q=1.57×1010J

Now the changes in entropies can be calculated as:

For earth:

role="math" localid="1647244335644" ΔSearth=QTearth

By substituting the values, we get,

ΔSearth=1.57×1010300ΔSearth=5.23×107JK-1

For sun:

role="math" localid="1647244543097" ΔSsun=-QTsun

By substituting the values, we get,

ΔSsun=-1.57×10106000ΔSsun=-2.62×106JK-1

We know that the net entropy change can be calculated as:

ΔStotal=ΔSsun+ΔSearth

By substituting the calculated values, we get,

ΔStotal=5.23×107-2.62×106ΔStotal=4.97×107JK-1

03

Part (a) Step 3: Final answer

Hence, the total entropy change can be calculated as4.97×107JK-1.

04

Part (b) Step 1: Concept Introduction

Entropy is a measure of a system's randomness or disorder in general. The total entropy can't be reduced, but it can stay the same if the processes are reversible, according to the law of thermodynamics.

05

Part (b) Step 2: Explanation

The second rule of thermodynamics is not violated by growing grass. This is due to its ability to harness solar energy and transform disordered molecules in the soil into an organized life. However, in the event of a biological reaction, entropy would be substantially lower, and hence far lower than the entropy caused by transporting energy from the Sun to the Earth.

06

Part (b) Step 3: Final answer

The entropy produced by transmitting energy from the sun to earth (disordered) would be far more than the entropy produced by biological reactions (ordered) in the grass, hence the development of grass does not break the second law of thermodynamics.

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Most popular questions from this chapter

Suppose you have a mixture of gases (such as air, a mixture of nitrogen and oxygen). The mole fraction xiof any species iis defined as the fraction of all the molecules that belong to that species: xi=Ni/Ntotal. The partial pressure Piof species iis then defined as the corresponding fraction of the total pressure: Pi=xiP. Assuming that the mixture of gases is ideal, argue that the chemical potential μiof species i in this system is the same as if the other gases were not present, at a fixed partial pressure Pi.

What partial-derivative relation can you derive from the thermodynamic identity by considering a process that takes place at constant entropy? Does the resulting equation agree with what you already knew? Explain.

In Section 2.5 I quoted a theorem on the multiplicity of any system with only quadratic degrees of freedom: In the high-temperature limit where the number of units of energy is much larger than the number of degrees of freedom, the multiplicity of any such system is proportional to UNf/2, whereNf is the total number of degrees of freedom. Find an expression for the energy of such a system in terms of its temperature, and comment on the result. How can you tell that this formula forΩ cannot be valid when the total energy is very small?

Polymers, like rubber, are made of very long molecules, usually tangled up in a configuration that has lots of entropy. As a very crude model of a rubber band, consider a chain of N links, each of length (see Figure 3.17). Imagine that each link has only two possible states, pointing either left or right. The total length L of the rubber band is the net displacement from the beginning of the first link to the end of the last link.

(a) Find an expression for the entropy of this system in terms of N and NR, the number of links pointing to the right.
(b) Write down a formula for L in terms of N and NR.
(c) For a one-dimensional system such as this, the length L is analogous to the volume V of a three-dimensional system. Similarly, the pressure P is replaced by the tension force F. Taking F to be positive when the rubber band is pulling inward, write down and explain the appropriate thermodynamic identity for this system.
(d) Using the thermodynamic identity, you can now express the tension force F in terms of a partial derivative of the entropy. From this expression, compute the tension in terms of L, T, N, and .
(e) Show that when L << N, the tension force is directly proportional to L (Hooke's law).
(f) Discuss the dependence of the tension force on temperature. If you increase the temperature of a rubber band, does it tend to expand or contract? Does this behavior make sense?
(g) Suppose that you hold a relaxed rubber band in both hands and suddenly stretch it. Would you expect its temperature to increase or decrease? Explain. Test your prediction with a real rubber band (preferably a fairly heavy one with lots of stretch), using your lips or forehead as a thermometer. (Hint: The entropy you computed in part (a) is not the total entropy of the rubber band. There is additional entropy associated with the vibrational energy of the molecules; this entropy depends on U but is approximately independent of L.)

Starting with the result of Problem 2.17, find a formula for the temperature of an Einstein solid in the limit qN. Solve for the energy as a function of temperature to obtain U=Nϵe-ϵ/kT (whereϵ is the size of an energy unit).

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