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Calculate the Compton wavelength for

(a) an electron and

(b) a proton. What is the photon energy for an electromagnetic wave with a wavelength equal to the Compton wavelength of

(c) the electron and

(d) the proton.

Short Answer

Expert verified

Thus, (a) the Compton wavelength for an electron is2.43鈥塸尘.

(b) The Compton wavelength for a proton is 1.32鈥塮尘.

(c) The energy for the electron is 0.511鈥塎别痴.

(d) The energy for the proton is939鈥塎别痴.

Step by step solution

01

The Compton wavelength for an electron.

(a)

The mass of an electron is m=9.1091031kg, its Compton wavelength is solved as follows:

C=hmc=6.6261034J.s(9.1091031kg)(2.998108m/s)=2.4261012m=2.43鈥塸尘

Hence, the Compton wavelength for an electron is2.43鈥塸尘 .

02

The Compton wavelength for a proton.

(b)

The mass of a proton ism=1.6731027kg, its Compton wavelength is solved as follows:

C=hmc=6.6261034J.s(1.6731027kg)(2.998108m/s)=1.3211015m=1.32鈥塮尘

Hence, the Compton wavelength for a proton is 1.32鈥塮尘.

03

 Step 3: The photon energy of an electromagnetic wave in a wavelength equal to the wavelength of an electron.

(c)

Let hc=1240鈥塭痴nmthen it gives,

E=hc=1240鈥塶尘eV

Here, E is the energy and is the wavelength.

Thus, the energy for the electron is;

E=1240鈥塶尘eV2.426103nm=5.11105eV=0.511鈥塎别痴

Hence, the energy for the electron is0.511鈥塎别痴 .

04

The photon energy of an electromagnetic wave in a wavelength equal to the wavelength of a proton

(d)

Let hc=1240鈥塭痴nmthen it gives,

E=hc=1240鈥塶尘eV

Here, E is the energy and is the wavelength.

Thus, the energy for the proton is;

E=1240鈥塶尘eV1.321106鈥塶尘=9.39108eV=939鈥塎别痴

Hence, the energy for the proton is939鈥塎别痴 .

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Most popular questions from this chapter

Question: You will find in Chapter 39 that electrons cannot move in definite orbits within atoms, like the planets in our solar system. To see why, let us try to 鈥渙bserve鈥 such an orbiting electron by using a light microscope to measure the electron鈥檚 presumed orbital position with a precision of, say, 10pm(a typical atom has a radius of about localid="1663132292844" 100pm). The wavelength of the light used in the microscope must then be about 10pm. (a) What would be the photon energy of this light? (b) How much energy would such a photon impart to an electron in a head-on collision? (c) What do these results tell you about the possibility of 鈥渧iewing鈥 an atomic electron at two or more points along its presumed orbital path? (Hint:The outer electrons of atomsare bound to the atom by energies of only a few electron-volts.)

Derive Eq. 38-11, the equation for the Compton shift, from Eqs. 38-8, 38-9, and 38-10 by eliminating v and .

Question:The uncertainty in the position of an electron along an xaxis

is given as 50pm, which is about equal to the radius of a hydrogen

atom. What is the least uncertainty in any simultaneous measurement

of the momentum component of this electron?

X rays of wavelength 0.0100 nm are directed in the positive direction of an x axis onto a target containing loosely bound electrons. For Compton scattering from one of those electrons, at an angle of , what are

(a) the Compton shift,

(b) the corresponding change in photon energy,

(c) the kinetic energy of the recoiling electron, and

(d) the angle between the positive direction of the x axis and the electron鈥檚 direction of motion?

What are

(a) the Compton shift ,

(b) the fractional Compton shift , and

(c) the changeE in photon energy for light of wavelength =590nmscattering from a free, initially stationary electron if the scattering is at to the direction of the incident beam? What are

(d) ,

(e) , and

(f) Efor90 scattering for photon energy 50.0 keV (x-ray range)?

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