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_1 and (c) the energy E1_1 associated with the first photon? What are (d) λ2_2 and (e) E2_2 associated with the second photon?

1360823-Figure 40.14
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(a) and (b) Let the wavelength of the two photons be λ1_1 and λ2=λ1+Δλ \lambda_2=\lambda_1+\Delta \lambda . Then,

eV=hcλ1+hcλ1+Δλλ1=(Δλ/λ02)±(Δλ/λ0)2+42/Δλ. e V=\frac{h c}{\lambda_1}+\frac{h c}{\lambda_1+\Delta \lambda} \Rightarrow \lambda_1=\frac{-\left(\Delta \lambda / \lambda_0-2\right) \pm \sqrt{\left(\Delta \lambda / \lambda_0\right)^2+4}}{2 / \Delta \lambda} .

Here, Δλ = 130 pm and

λ0=hc/eV=1240keVpm/20keV=62pm \lambda_0=h c / e V=1240 \, keV \cdot pm / 20\, keV =62\, pm ,

where we have used hc = 1240 eV·nm = 1240 keV·pm. We choose the plus sign in the expression for λ1_1 (since λ1_1 > 0) and obtain

λ1=(130pm/62pm2)+(130pm/62pm)2+42/62pm=87pm. \lambda_1=\frac{-(130 \,pm / 62 \,pm -2)+\sqrt{(130 \,pm / 62\, pm )^2+4}}{2 / 62 \,pm }=87 \,pm .

The energy of the electron after its first deceleration is

K=Kihcλ1=20keV1240keVpm87pm=5.7keV K=K_i-\frac{h c}{\lambda_1}=20 \,keV -\frac{1240 \,keV \cdot pm }{87 \,pm }=5.7 \,keV .

(c) The energy of the first photon is E1=hcλ1=1240keVpm87pm=14keV E_1=\frac{h c}{\lambda_1}=\frac{1240 \,keV \cdot pm }{87 \,pm }=14 \,keV .

(d) The wavelength associated with the second photon is

λ2=λ1+Δλ=87pm+130pm=2.2×102pm. \lambda_2=\lambda_1+\Delta \lambda=87 \,pm +130 \,pm =2.2 \times 10^2 \,pm .

(e) The energy of the second photon is E2=hcλ2=1240keVpm2.2×102pm=5.7keV E_2=\frac{h c}{\lambda_2}=\frac{1240 \,keV \cdot pm }{2.2 \times 10^2 \,pm }=5.7 \,keV .

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