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

Consider a system consisting of a single impurity atom/ion in a semiconductor. Suppose that the impurity atom has one "extra" electron compared to the neighboring atoms, as would a phosphorus atom occupying a lattice site in a silicon crystal. The extra electron is then easily removed, leaving behind a positively charged ion. The ionized electron is called a conduction electron, because it is free to move through the material; the impurity atom is called a donor, because it can "donate" a conduction electron. This system is analogous to the hydrogen atom considered in the previous two problems except that the ionization energy is much less, mainly due to the screening of the ionic charge by the dielectric behavior of the medium.

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(a) Explain why, if g0vg0c, the chemical potential will now vary with temperature. When will it increase, and when will it decrease?

(b) Write down an expression for the number of conduction electrons, in terms of T,μ,candg0cSimplify this expression as much as possible, assuming ϵc-μkT.

(c) An empty state in the valence band is called a hole. In analogy to part (b), write down an expression for the number of holes, and simplify it in the limit μ-ϵvkT.

(d) Combine the results of parts (b) and (c) to find an expression for the chemical potential as a function of temperature.

(e) For silicon, g0cg0=1.09andg0vg0=0.44*.Calculate the shift inµ for silicon at room temperature.

Near the cells where oxygen is used, its chemical potential is significantly lower than near the lungs. Even though there is no gaseous oxygen near these cells, it is customary to express the abundance of oxygen in terms of the partial pressure of gaseous oxygen that would be in equilibrium with the blood. Using the independent-site model just presented, with only oxygen present, calculate and plot the fraction of occupied heme sites as a function of the partial pressure of oxygen. This curve is called the Langmuir adsorption isotherm ("isotherm" because it's for a fixed temperature). Experiments show that adsorption by myosin follows the shape of this curve quite accurately.

Consider a system consisting of a single impurity atom/ion in a semiconductor. Suppose that the impurity atom has one "extra" electron compared to the neighboring atoms, as would a phosphorus atom occupying a lattice site in a silicon crystal. The extra electron is then easily removed, leaving behind a positively charged ion. The ionized electron is called a conduction electron because it is free to move through the material; the impurity atom is called a donor, because it can "donate" a conduction electron. This system is analogous to the hydrogen atom considered in the previous two problems except that the ionization energy is much less, mainly due to the screening of the ionic charge by the dielectric behavior of the medium.

(a) Write down a formula for the probability of a single donor atom being ionized. Do not neglect the fact that the electron, if present, can have two independent spin states. Express your formula in terms of the temperature, the ionization energy I, and the chemical potential of the "gas" of ionized electrons.

(b) Assuming that the conduction electrons behave like an ordinary ideal gas (with two spin states per particle), write their chemical potential in terms of the number of conduction electrons per unit volume,NcV.

(c) Now assume that every conduction electron comes from an ionized donor atom. In this case the number of conduction electrons is equal to the number of donors that are ionized. Use this condition to derive a quadratic equation for Ncin terms of the number of donor atoms Nd, eliminatingµ. Solve for Ncusing the quadratic formula. (Hint: It's helpful to introduce some abbreviations for dimensionless quantities. Tryx=NcNd,t=kTland so on.)

(d) For phosphorus in silicon, the ionization energy is localid="1650039340485" 0.044eV. Suppose that there are 1017patoms per cubic centimeter. Using these numbers, calculate and plot the fraction of ionized donors as a function of temperature. Discuss the results.

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