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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

In Problem 7.28you found the density of states and the chemical potential for a two-dimensional Fermi gas. Calculate the heat capacity of this gas in the limit role="math" localid="1650099524353" kT≪εF· Also show that the heat capacity has the expected behavior when kT≫εF. Sketch the heat capacity as a function of temperature.

Repeat the previous problem, taking into account the two independent spin states of the electron. Now the system has two "occupied" states, one with the electron in each spin configuration. However, the chemical potential of the electron gas is also slightly different. Show that the ratio of probabilities is the same as before: The spin degeneracy cancels out of the Saha equation.

A black hole is a blackbody if ever there was one, so it should emit blackbody radiation, called Hawking radiation. A black hole of mass M has a total energy of Mc2, a surface area of 16Ï€G2M2/c4, and a temperature ofhc3/16Ï€2kGM(as shown in Problem 3.7).

(a) Estimate the typical wavelength of the Hawking radiation emitted by a one-solar-mass (2 x 1030 kg) black hole. Compare your answer to the size of the black hole.

(b) Calculate the total power radiated by a one-solar-mass black hole.

(c) Imagine a black hole in empty space, where it emits radiation but absorbs nothing. As it loses energy, its mass must decrease; one could say it "evaporates." Derive a differential equation for the mass as a function of time, and solve this equation to obtain an expression for the lifetime of a black hole in terms of its initial mass.

(d) Calculate the lifetime of a one-solar-mass black hole, and compare to the estimated age of the known universe (1010 years).

(e) Suppose that a black hole that was created early in the history of the universe finishes evaporating today. What was its initial mass? In what part of the electromagnetic spectrum would most of its radiation have been emitted?

In the text I claimed that the universe was filled with ionised gas until its temperature cooled to about 3000 K. To see why, assume that the universe contains only photons and hydrogen atoms, with a constant ratio of 109 photons per hydrogen atom. Calculate and plot the fraction of atoms that were ionised as a function of temperature, for temperatures between 0 and 6000 K. How does the result change if the ratio of photons to atoms is 108 or 1010? (Hint: Write everything in terms of dimensionless variables such as t = kT/I, where I is the ionisation energy of hydrogen.)

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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