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

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 Bose gas confined in an isotropic harmonic trap, as in the previous problem. For this system, because the energy level structure is much simpler than that of a three-dimensional box, it is feasible to carry out the sum in equation 7.121 numerically, without approximating it as an integral.*

(a) Write equation 7.121 for this system as a sum over energy levels, taking degeneracy into account. Replace Tandμwith the dimensionless variables t=kT/hfandc=μ/hf.

(b) Program a computer to calculate this sum for any given values of tandc. Show that, for N=2000, equation 7.121 is satisfied at t=15provided that c=-10.534. (Hint: You'll need to include approximately the first 200 energy levels in the sum.)

(c) For the same parameters as in part (b), plot the number of particles in each energy level as a function of energy.

(d) Now reduce tto 14 , and adjust the value of cuntil the sum again equals 2000. Plot the number of particles as a function of energy.

(e) Repeat part (d) for t=13,12,11,and10. You should find that the required value of cincreases toward zero but never quite reaches it. Discuss the results in some detail.

Each atom in a chunk of copper contributes one conduction electron. Look up the density and atomic mass of copper, and calculate the Fermi energy, the Fermi temperature, the degeneracy pressure, and the contribution of the degeneracy pressure to the bulk modulus. Is room temperature sufficiently low to treat this system as a degenerate electron gas?

Suppose you have a "box" in which each particle may occupy any of 10single-particle states. For simplicity, assume that each of these states has energy zero.

(a) What is the partition function of this system if the box contains only one particle?

(b) What is the partition function of this system if the box contains two distinguishable particles?

(c) What is the partition function if the box contains two identical bosons?

(d) What is the partition function if the box contains two identical fermions?

(e) What would be the partition function of this system according to equation 7.16?

(f) What is the probability of finding both particles in the same single particle state, for the three cases of distinguishable particles, identical bosom, and identical fermions?

For a system of fermions at room temperature, compute the probability of a single-particle state being occupied if its energy is

(a) 1eVless than μ

(b) 0.01eVless than μ

(c) equal to μ

(d) 0.01eVgreater than μ

(e) 1eVgreater thanμ

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