366 Chapter 12Second-order differential equations. Constant coefficients
21.Solve subject to the conditionθ(t 1 + 12 πτ) 1 = 1 θ(t).
Section 12.5
22.Given that the general solution of the equation of motionmP1= 1 −kxfor the harmonic
oscillator isx(t) 1 = 1 a 1 cos 1 ωt 1 + 1 b 1 sin 1 ωt, where , (i)show that the solution can be
written in the formx(t) 1 = 1 A 1 cos(ωt 1 − 1 δ), where Ais the amplitude of the vibration and δ
is the phase angle, and express Aand δin terms of aand b; (ii)find the amplitude and
phase angle for the initial conditionsx(0) 1 = 11 , H(0) 1 = 1 ω.
23.Solve the equation of motion for the harmonic oscillator with initial conditionsx(0) 1 = 10 ,
H(0) 1 = 1 u
0
.
Section 12.6
24.For the particle in a box, find the nodes and sketch the graph of the wave functionψ
nfor
(i)n 1 = 14 and (ii)n 1 = 15.
- (i) Solve the Schrödinger equation (12.44) for the particle in a box of length lwith
potential-energy functionV 1 = 10 for−l 221 ≤ 1 x 1 ≤ 1 +l 22 , V 1 = 1 ∞forx 1 ≤ 1 −l 22 andx 1 ≥ 1 +l 22.
(ii) Show that the solutionsψ
nare even functions of xwhen nis odd and odd functions
when nis even. (iii) Show that the solutions are the same as those given by (12.53) if xis
replaced byx 1 + 1 l 22 , except for a possible change of sign.
26.For the particle in the box in Section 12.6, show that wave functions
forn 1 = 11 andn 1 = 12 are (i)normalized, (ii)orthogonal.
Section 12.7
27.For the particle in a ring show that wave functions forn 1 = 13 and
n 1 = 14 are (i)normalized, (ii)orthogonal.
28.The diagrams of Figure 12.8 are maps of the signs and nodes of some real wave functions
(12.71) for the particle in a ring. Draw the corresponding diagrams for (i) n 1 = 1 ± 3 ,
(ii)n 1 = 1 ± 4.
29.Verify that equation (12.72) and its solutions (12.74) are transformed into (12.62) and
(12.65) by means of the change of variableθ 1 = 1 x 2 r.
Section 12.8
30.Find a particular solution of the differential equationy′′ 1 − 1 y′ 1 − 16 y 1 = 121 + 13 x.
Find the general solutions of the differential equations:
31.y′′ 1 − 1 y′ 1 − 16 y 1 = 121 + 13 x 32.y′′ 1 − 18 y′ 1 + 116 y 1 = 111 − 14 x
3
33.y′′ 1 − 1 y′ 1 − 16 y 1 = 12 e
− 3 x34.y′′ 1 − 1 y′ 1 − 12 y 1 = 13 e
−x35.y′′ 1 − 18 y′ 1 + 116 y 1 = 1 e
4 x36.y′′ 1 − 1 y′ 1 − 16 y 1 = 121 cos 13 x
37.y′′ 1 + 14 y 1 = 131 sin 12 x 38.y′′ 1 − 1 y′ 1 − 16 y 1 = 121 + 13 x 1 + 12 e
− 3 x1 + 121 cos 13 x
Section 12.9
39.An RLC-circuit contains a resistor (resistance R), an inductor (inductance L), and a
capacitor (capacitance C) connected in series with a source of e.m.f. E.
ψ θ
θnin()= 12 πe
ψ
nx
l
nx
l
() sin=
2 π
ω= km
d
dt
a
2
2
2
0
θ
+=θ
dy
dx
dy
dx
yy y x
2
2
+−=;20 02 0()=,→ as →∞