Explain to your friend, who is skeptical about energy quantization, the simple evidence provided by distinct colors you see when you hold a CD (serving as grating) near a fluorescent light. It may be helpful to contrast this evidence with the spectrum produced by an incandescent light, which relies on heating to produce a rather nonspecific blackbody spectrum.

Short Answer

Expert verified

The discrete colors seen when you look at a CD are a direct evidence of energy quantization because the color of light that we see depends on its wavelength, which is related to its energy. If the energy is quantized, the wavelengths of the light are discrete so we see discrete colors (not white light as in case of a light bulb).

Step by step solution

01

Given data

If E is discrete, wavelength is discrete.

02

 Step 2: Concept of wavelength of electromagnetic radiation

The wavelength of an electromagnetic radiation is related to its energy by relation:

E=hcλ

Where, his the Planck's constant, cis the speed of light,λis the wavelength and Eis the energy.

03

Diffraction of light

A CD has tiny grooves on it. Based on the size of the grooves, certain wavelengths of the light are diffracted by the CD in different directions. A fluorescent light source emits only certain wavelengths. So, when we look at a CD, illuminated by a fluorescent light source, we see only the wavelength that is diffracted at an angle towards our eye. If the wavelengths were not discrete, we would see multiple wavelengths at a time from the same spot on the CD resulting in white color.

04

Incandescent light source

You don't see colors when you illuminate the CD by an incandescent light source. This is because, the wavelengths emitted by an incandescent light source are not discrete, they are continuous and their intensity depends on the temperature of the heating filament. Continuous means all wavelengths are present. You cannot say that this particular wavelength is absent in this incandescent light source.

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

Calculate the uncertainty in the particle’s position.

Summarize the similarities are differences between the three simple bound cases considered in this chapter.

Show thatΔp=0p^ψ(x)=p¯ψ(x) that is, verify that unless the wave function is an Eigen function of the momentum operator, there will be a nonzero uncertainty in the momentumstarts with showing that the quantity

allspaceψ(x)(p^p¯)2ψ(x)dx

Is (Δp)2. Then using the differential operator form ofp^and integration by parts, show that it is also,

allspace{(p^p¯)ψ(x)}{(p^p¯)ψ(x)}dx

Together these show that ifΔpis. 0. then the preceding quantity must be 0. However, the Integral of the complex square of a function(the quantity in the brackets) can only be 0 if the function is identically 0, so the assertion is proved.

To determine the classical expectation value of the position of a particle in a box is L2 , the expectation value of the square of the position of a particle in a box isrole="math" localid="1658324625272" L23 , and the uncertainty in the position of a particle in a box isL12 .

If a particle in a stationary state is bound, the expectation value of its momentum must be 0.

(a). In words, why?

(b) Prove it.

Starting from the general expression(5-31) with p^in the place of Q, integrate by parts, then argue that the result is identically 0. Be careful that your argument is somehow based on the particle being bound: a free particle certainly may have a non zero momentum. (Note: Without loss of generality,ψ(x) may be chosen to be real.)

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