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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.

Short Answer

Expert verified

Hence, the pressure exerted inside a kiln isP=1.272×10-3Pa

Step by step solution

01

Given information

Formula to be used isP=-(∂U/∂V)S,N

02

Explanation

At constant N and S, the pressure equals the negative of the partial derivative of the total energy with respect to the volume, i.e.

P=-∂U∂VN,S(1)

To calculate the pressure, we must express the total energy in terms of entropy. The total energy is calculated as follows:

U=8Ï€5(kT)415(hc)3V

The entropy is given as:

S=32Ï€545VkThc3k

Let

A=8Ï€2k415(hc)3

Total energy and entropy is:

U=AVT4andS=43AVT3

Solve entropy equation for T:

T=3S4AV1/3

Substitute T in total energy:

U=AV3S4AV4/3U=A3S4A4/31V1/3

Substitute in equation (1)

P=-A3S4A4/3∂∂V1V1/3P=-A3S4A4/3-131V4/3P=13A3S4AV4/3

But,

T=3S4AV1/3

Therefore,

P=13AT4

03

Explanation

The total energy of radiation is:

U=8Ï€5(kT)415(hc)3V

Substitute the values:

UV=8π51.38×10-23J/K(1500K)4156.626×10-34J·s3.0×108m/s3=3.815×10-3J/m3

The pressure is:

P=133.815×10-3J/m3=1.272×10-3J/m3=1.272×10-3PaP=1.272×10-3Pa

For comparison, the pressure within the kiln is the same as the pressure outside it, which is 1 atm in pascal 1.01 x 105 Pa, which is about 108 higher than the pressure caused by photons. The temperature at the sun's core is T = 15 x 106 K, hence the energy per unit volume is:

UV=8π51.38×10-23J/K15×106K4156.626×10-34J·s3.0×108m/s3=3.815×1013J/m3

The pressure is:

role="math" localid="1647764290491" P=133.815×1013J/m3=1.272×1013J/m3=1.272×1013PaP=1.272×1013Pa

Number of moles per unit volume equals to:

nV=103mole/kg105kg/m3=108mole/m3

The pressure is:

P=nRTV=2108mole/m3(8.314J/K·mole)15×106K=2.5×1016Pa

The factor 2 came from the fact that each ionised hydrogen atom has and electron and a proton.

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Most popular questions from this chapter

Show that when a system is in thermal and diffusive equilibrium with a reservoir, the average number of particles in the system is

N—=kTZ∂Z∂μ

where the partial derivative is taken at fixed temperature and volume. Show also that the mean square number of particles is

N2¯=(kT)2Z∂2Z∂μ2

Use these results to show that the standard deviation of Nis

σN=kT∂N—/∂μ,

in analogy with Problem6.18Finally, apply this formula to an ideal gas, to obtain a simple expression forσNin terms ofN¯Discuss your result briefly.

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B=probability of absorption per unit timeu(f)

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As Einstein showed in 1917, knowing any one of these three coefficients is as good as knowing them all.

(a) Imagine a collection of many of these atoms, such that N1 of them are in state s1 and N2 are in state s2. Write down a formula for dN1/dt in terms of A, B, B', N1, N2, and u(f).

(b) Einstein's trick is to imagine that these atoms are bathed in thermal radiation, so that u(f) is the Planck spectral function. At equilibrium, N1and N2 should be constant in time, with their ratio given by a simple Boltzmann factor. Show, then, that the coefficients must be related by

B'=BandAB=8Ï€hf3c3

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(a) Describe the ground state of this system, for each of these three cases.

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