636 14 Classical Mechanics and the Old Quantum Theory
10
n 53
n 52n 51
Sum of
3 harmonics0.0 0.2 0.4
x/L
(a)0.6 0.8 1.0Wave displacement2110n 53n 52n 51Sum of
3 harmonics0.0 0.2 0.4
x/L
(b)0.6 0.8 1.0Wave displacement21Figure 14.8 The Superposition of Three Harmonics of a Flexible String.(a) At time
tL/ 4 c. (b) At timet 3 L/ 4 c.t0, the following linear combination is a solution of the wave equationz(x,t)∑∞
n 1Ansin(nπx
L)
sin(nπct
L)
(14.3-25)
whereA 1 ,A 2 ,...are constants.Exercise 14.7
Show by substitution that the series in Eq. (14.3-25) satisfies Eq. (14.3-3).The different harmonics exhibit constructive interference and destructive interference
that continually change, because the different harmonics have different frequencies.
Figure 14.8 shows a linear combination of three harmonics withA 1 1,A 2  0 .2,
andA 3  0 .1. Figure 14.8a shows the sum at timetL/(4c), and Figure 14.8b shows
the sum att 3 L/(4c).Traveling Waves
In a string of finite length with stationary ends, only standing waves can occur. Traveling
waves can occur in a very long string. A wave function that satisfies Eq. (14.3-3) and
corresponds to a traveling wave isz(x,t)Asin(κx−κct) (14.3-26)Exercise 14.8
Show by substitution that the function in Eq. (14.3-26) satisfies Eq. (14.3-3).