p41 049

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49.

(a) An electron must be removed from the K-shell, so that an electron from a higher energy shell can

drop. This requires an energy of 69.5keV. The accelerating potential must be at least 69.5kV.

(b) After it is accelerated, the kinetic energy of the bombarding electron is 69.5keV. The energy of a

photon associated with the minimum wavelength is 69.5keV, so its wavelength is

λ

min

=

1240 eV

·nm

69.5

× 10

3

eV

= 1.78

× 10

2

nm = 17.8 pm .

(c) The energy of a photon associated with the K

α

line is 69.5keV

11.3 keV = 5 8.2 keV and its

wavelength is λ

Kα

= (1240 eV

·nm)/(58.2 × 10

3

eV) = 2.13

× 10

2

nm = 21.3 pm. The energy

of a photon associated with the K

β

line is 69.5keV

2.30 keV = 67.2 keV and its wavelength is

λ

Kβ

= (1240 eV

·nm)/(67.2 × 10

3

eV) = 1.85

× 10

2

nm = 18.5pm. The result of Exercise 3 of

Chapter 39 is used.


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