A 20 keV electron is brought to rest by colliding twice with target nuclei as in Fig. 40-14. (Assume the nuclei remain stationary.) The wavelength associated with the photon emitted in the second collision is 130 pm greater than that associated with the photon emitted in the first collision. (a) What is the kinetic energy of the electron after the first collision? What are (b) the wavelength λ1 and (c) the energy E1 associated with the first photon? What are (d) λ2 and (e) E2 associated with the second photon?
(a) and (b) Let the wavelength of the two photons be λ1 and λ2=λ1+Δλ. Then,
eV=λ1hc+λ1+Δλhc⇒λ1=2/Δλ−(Δλ/λ0−2)±(Δλ/λ0)2+4.
Here, Δλ = 130 pm and
λ0=hc/eV=1240keV⋅pm/20keV=62pm,
where we have used hc = 1240 eV·nm = 1240 keV·pm. We choose the plus sign in the expression for λ1 (since λ1 > 0) and obtain
λ1=2/62pm−(130pm/62pm−2)+(130pm/62pm)2+4=87pm.
The energy of the electron after its first deceleration is
K=Ki−λ1hc=20keV−87pm1240keV⋅pm=5.7keV.
(c) The energy of the first photon is E1=λ1hc=87pm1240keV⋅pm=14keV.
(d) The wavelength associated with the second photon is
λ2=λ1+Δλ=87pm+130pm=2.2×102pm.
(e) The energy of the second photon is E2=λ2hc=2.2×102pm1240keV⋅pm=5.7keV.