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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=-UVN,S(1)

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

U=8π5(kT)415(hc)3V

The entropy is given as:

S=32π545VkThc3k

Let

A=8π2k415(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=-A3S4A4/3V1V1/3P=-A3S4A4/3-131V4/3P=13A3S4AV4/3

But,

T=3S4AV1/3

Therefore,

P=13AT4

03

Explanation

The total energy of radiation is:

U=8π5(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

Figure 7.37 shows the heat capacity of a Bose gas as a function of temperature. In this problem you will calculate the shape of this unusual graph.

(a) Write down an expression for the total energy of a gas of Nbosons confined to a volume V, in terms of an integral (analogous to equation 7.122).

(b) For T<Tcyou can set μ=0. Evaluate the integral numerically in this case, then differentiate the result with respect to Tto obtain the heat capacity. Compare to Figure 7.37.

(c) Explain why the heat capacity must approach 32Nkin the high- Tlimit.

(d) For T>Tcyou can evaluate the integral using the values of μcalculated in Problem 7.69. Do this to obtain the energy as a function of temperature, then numerically differentiate the result to obtain the heat capacity. Plot the heat capacity, and check that your graph agrees with Figure 7.37.

Figure 7.37. Heat capacity of an ideal Bose gas in a three-dimensional box.

It's not obvious from Figure 7.19 how the Planck spectrum changes as a function of temperature. To examine the temperature dependence, make a quantitative plot of the functionu(ϵ) for T = 3000 K and T = 6000 K (both on the same graph). Label the horizontal axis in electron-volts.

A star that is too heavy to stabilize as a white dwarf can collapse further to form a neutron star: a star made entirely of neutrons, supported against gravitational collapse by degenerate neutron pressure. Repeat the steps of the previous problem for a neutron star, to determine the following: the mass radius relation; the radius, density, Fermi energy, and Fermi temperature of a one-solar-mass neutron star; and the critical mass above which a neutron star becomes relativistic and hence unstable to further collapse.

Consider a gas of noninteracting spin-0 bosons at high temperatures, when TTc. (Note that “high” in this sense can still mean below 1 K.)

  1. Show that, in this limit, the Bose-Einstein function can be written approximately as
    n¯BE=e(μ)/kT[1+eμ/kT+].
  2. Keeping only the terms shown above, plug this result into equation 7.122 to derive the first quantum correction to the chemical potential for gas of bosons.
  3. Use the properties of the grand free energy (Problems 5.23 and 7.7) to show that the pressure of any system is given by In P=(kT/V), where Zis the grand partition function. Argue that, for gas of noninteracting particles, In Zcan be computed as the sum over all modes (or single-particle states) of In Zi, where Zi; is the grand partition function for the ithmode.
  4. Continuing with the result of part (c), write the sum over modes as an integral over energy, using the density of states. Evaluate this integral explicitly for gas of noninteracting bosons in the high-temperature limit, using the result of part (b) for the chemical potential and expanding the logarithm as appropriate. When the smoke clears, you should find
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  5. Write the result of part (d) in the form of the virial expansion introduced in Problem 1.17, and read off the second virial coefficient, B(T). Plot the predicted B(T)for a hypothetical gas of noninteracting helium-4 atoms.
  6. Repeat this entire problem for gas of spin-1/2 fermions. (Very few modifications are necessary.) Discuss the results, and plot the predicted virial coefficient for a hypothetical gas of noninteracting helium-3 atoms.

For a brief time in the early universe, the temperature was hot enough to produce large numbers of electron-positron pairs. These pairs then constituted a third type of "background radiation," in addition to the photons and neutrinos (see Figure 7.21). Like neutrinos, electrons and positrons are fermions. Unlike neutrinos, electrons and positrons are known to be massive (ea.ch with the same mass), and each has two independent polarization states. During the time period of interest, the densities of electrons and positrons were approximately equal, so it is a good approximation to set the chemical potentials equal to zero as in Figure 7.21. When the temperature was greater than the electron mass times c2k, the universe was filled with three types of radiation: electrons and positrons (solid arrows); neutrinos (dashed); and photons (wavy). Bathed in this radiation were a few protons and neutrons, roughly one for every billion radiation particles. the previous problem. Recall from special relativity that the energy of a massive particle is ϵ=(pc)2+mc22.

(a) Show that the energy density of electrons and positrons at temperature Tis given by

u(T)=0x2x2+mc2/kT2ex2+mc2/kT2+1dx;whereu(T)=0x2x2+mc2/kT2ex2+mc2/kT2+1dx

(b) Show that u(T)goes to zero when kTmc2, and explain why this is a

reasonable result.

( c) Evaluate u(T)in the limit kTmc2, and compare to the result of the

the previous problem for the neutrino radiation.

(d) Use a computer to calculate and plot u(T)at intermediate temperatures.

(e) Use the method of Problem 7.46, part (d), to show that the free energy

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Evaluate f(T)in both limits, and use a computer to calculate and plot f(T)at intermediate

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(f) Write the entropy of the electron-positron radiation in terms of the functions

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