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
n
for
(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
n
are 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 x
34.y′′ 1 − 1 y′ 1 − 12 y 1 = 13 e
−x
35.y′′ 1 − 18 y′ 1 + 116 y 1 = 1 e
4 x
36.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 x
1 + 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
θ
n
in
()= 12 πe
ψ
n
x
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 →∞