The temperature of our Sun’s surface is ~6000K.(a) At what wavelength is the spectral emission of the Sun is maximum? (Refer to Exercise 79.) (b) Is there something conspicuous about this wavelength?

Short Answer

Expert verified

(a) The wavelength at which the spectral emission is maximum is4.828×10-7m .

(b) It is conspicuous as it is in the visible range of the spectrum.

Step by step solution

01

Given data

Given data can be listed below as:

The temperature of the sun is, T=6000K.T=6000K.

02

Wein’s displacement law

The law gives the relationship between the maximum wavelength of the radiation that was released from a black body and the temperature at which the black body was kept; this relationship can be expressed as,

λmaxT=b (1)

Here λmaxis the maximum wavelength, localid="1660183413143" Tis the temperature at which the black body was kept, and localid="1660183425059" bis known as Wien’s displacement constant.

03

a) Determination of Wavelength for the maximum temperature of the sun

Let’s modify equation 1 as,

λmax=bT (2)

The value of Wien’s displacement constant is, b=2.897×10-3m·K.

The wavelength at which the spectral emission of the Sun is maximum can be calculated from the above expression. The maximum spectral emission is associated with the maximum wavelength (peak in the energy-temperature curve) for that given temperature.

Substitute the values in equation 2, and we get,

λmax=2.897×10-3m·K6000K=4.828×10-7m

Thus, the wavelength at which the spectral emission is maximum is 4.828×10-7m.

04

b) Conspicuous about this wavelength

From the calculation of part a, the wavelength at which the spectral emission is maximum is 4.828×10-7m.

The visible spectrum exists between 300nmand 700nm.

The wavelength we calculated in nm can be calculated as,

=4.828×10-7m=4.828×10-7·1m×109nm1m=4.828×10-7×109nm=4.828×102nm=482.8nm

This is between the visible range in the middle, to be precise.

Thus, it is conspicuous as it is in the visible range of the spectrum.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Classically, what would be the average energy of a particle in a system of particles fine to move in the xy-plane while rotating about the i-axis?

There is a simple argument, practically by inspection, that distributions(9-31),(9-32), and(9-33)should agree whenever occupation number is much less than 1. Provide the argument.

Copper has one conduction electron per atom and a density of8.9×103kg/m3. By the criteria of equation(943), show that at room temperature(300K), the conduction electron gas must be treated as a quantum gas of indistinguishable particles.

A scientifically untrained but curious friend asks, "When I walk into a room, is there a chance that all the air will be on the other side?" How do you answer this question?

The electrons’ contribution to the heat capacity of a metal is small and goes to 0as T0. We might try to calculate it via the total internal energy, localid="1660131882505" U=EN(E)D(E)dE, but it is one of those integrals impossible to do in closed form, and localid="1660131274621" N(E)FDis the culprit. Still, we can explain why the heat capacity should go to zero and obtain a rough value.

(a) Starting withN(E)FDexpressed as in equation (34), show that the slope N(E)FDdEatE=EFis-1(4kBT).

(b) Based on part (a), the accompanying figure is a good approximation to N(E)FDwhen Tis small. In a normal gas, such as air, whenTis raised a little, all molecules, on average, gain a little energy, proportional to kBT. Thus, the internal energy Uincreases linearly with T, and the heat capacity, UT, is roughly constant. Argue on the basis of the figure that in this fermion gas, as the temperature increases from 0to a small value T, while some particles gain energy of roughly kBT, not all do, and the number doing so is also roughly proportional to localid="1660131824460" T. What effect does this have on the heat capacity?

(c)Viewing the total energy increase as simply U= (number of particles whose energy increases) (energy change per particle) and assuming the density of states is simply a constant Dover the entire range of particle energies, show that the heat capacity under these lowest-temperature conditions should be proportional to kBREFT. (Trying to be more precise is not really worthwhile, for the proportionality constant is subject to several corrections from effects we ignore).

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free