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At the surface of the sun, the temperature is approximately 5800 K.

(a) How much energy is contained in the electromagnetic radiation filling a cubic meter of space at the sun's surface?

(b) Sketch the spectrum of this radiation as a function of photon energy. Mark the region of the spectrum that corresponds to visible wavelengths, between 400 nm and 700 nm.

(c) What fraction of the energy is in the visible portion of the spectrum? (Hint: Do the integral numerically.)

Short Answer

Expert verified

Therefore, the energy contained in electromagnetic radiation is

U=0.853J

Step by step solution

01

Given information

At the surface of the sun, the temperature is approximately 5800 K.

02

Explanation

(a)Assuming the sun's temperature is 5800 K,

The total energy of this radiation inside 1 cubic metre of sun is given by: sum V= 1m3, total energy of this radiation is given by

U=8π5(kT)415(hc)3V

Substitute the given values

U=8π51.38×10-23J/K(5800K)4156.626×10-34J·s3.0×108m/s31m3U=0.853J

(b) Spectrum of radiation is:

u(ϵ)=8π(hc)3ϵ3eϵ/kT-1

To sketch the above expression python is used and the code is:

The graph is:

03

Explanation

The energy in terms of wavelength is:

ϵ=hcλ

Therefore,

ϵ2=6.626×10-34J·s3.0×108m/s400×10-9m=4.9695×10-19J=3.1eVϵ1=6.626×10-34J·s3.0×108m/s700×10-9m=2.84×10-19J=1.77eV

The code used to mark the region of the visible light

(c)Now we need to discover the component of the spectrum that represents visible light (the fraction of the energy), which we can do by integrating the following equation all across the visible light (equation 785):

U=8πV(hc)3ϵ1ϵ2x3ex-1dx

Energy in terms of wavelength is:

ϵ=hcλ

Hence,

ϵ2=6.626×10-34J·s3.0×108m/s400×10-9m=4.9695×10-19J=3.1eVϵ1=6.626×10-34J·s3.0×108m/s700×10-9m=2.84×10-19J=1.77eV

Fraction of energy in visible light is:

Uvis.Utot.=1.77eV3.1eVx3ex-1dx0x3ex-1dx

Integration in denominator equals to π4/15, therefore

Uvis.Utot=15π41.77eV3.1eVx3ex-1dϵ

We have,

x=ϵkT

The temperature is T=1500K

x1=ϵ1kT=1.77eV8.62×10-5eV/K(5800K)=3.54x2=ϵ2kT=3.1eVeV8.62×10-5eV/K(5800K)=6.8

Hence the integral is:

Uvis.Utot.=15π43.546.8x3ex-1dϵ

To evaluate the integral, python is used, the code is given below and the ratio is:

Uvis.Utot.=0.382

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Most popular questions from this chapter

The argument given above for why CvTdoes not depend on the details of the energy levels available to the fermions, so it should also apply to the model considered in Problem 7.16: a gas of fermions trapped in such a way that the energy levels are evenly spaced and non-degenerate.

(a) Show that, in this model, the number of possible system states for a given value of q is equal to the number of distinct ways of writing q as a sum of positive integers. (For example, there are three system states for q = 3, corresponding to the sums 3, 2 + 1, and 1 + 1 + 1. Note that 2 + 1 and 1 + 2 are not counted separately.) This combinatorial function is called the number of unrestricted partitions of q, denoted p(q). For example, p(3) = 3.

(b) By enumerating the partitions explicitly, compute p(7) and p(8).

(c) Make a table of p(q) for values of q up to 100, by either looking up the values in a mathematical reference book, or using a software package that can compute them, or writing your own program to compute them. From this table, compute the entropy, temperature, and heat capacity of this system, using the same methods as in Section 3.3. Plot the heat capacity as a function of temperature, and note that it is approximately linear.

(d) Ramanujan and Hardy (two famous mathematicians) have shown that when q is large, the number of unrestricted partitions of q is given approximately by

p(q)eπ2q343q

Check the accuracy of this formula for q = 10 and for q = 100. Working in this approximation, calculate the entropy, temperature, and heat capacity of this system. Express the heat. capacity as a series in decreasing powers of kT/η, assuming that this ratio is large and keeping the two largest terms. Compare to the numerical results you obtained in part (c). Why is the heat capacity of this system independent of N, unlike that of the three dimensional box of fermions discussed in the text?

Use the formula P=-(U/V)S,N to show that the pressure of a photon gas is 1/3 times the energy density (U/V). Compute the pressure exerted by the radiation inside a kiln at 1500 K, and compare to the ordinary gas pressure exerted by the air. Then compute the pressure of the radiation at the centre of the sun, where the temperature is 15 million K. Compare to the gas pressure of the ionised hydrogen, whose density is approximately 105 kg/m3.

Evaluate the integral in equation N=2π2πmh23/2V0ϵdϵeϵ/kT-1numerically, to confirm the value quoted in the text.

The Sommerfeld expansion is an expansion in powers of kTεF, which is assumed to be small. In this section I kept all terms through order kTεF2, omitting higher-order terms. Show at each relevant step that the term proportional to localid="1650117451748" T3is zero, so that the next nonvanishing terms in the expansions forlocalid="1650117470867" μand localid="1650117476821" Uare proportional to localid="1650117458596" T4. (If you enjoy such things, you might try evaluating the localid="1650117464980" T4terms, possibly with the aid of a computer algebra program.)

Compute the quantum volume for an N2molecule at room temperature, and argue that a gas of such molecules at atmospheric pressure can be

treated using Boltzmann statistics. At about what temperature would quantum statistics become relevant for this system (keeping the density constant and pretending that the gas does not liquefy)?

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