636 14 Classical Mechanics and the Old Quantum Theory
1
0
n 53
n 52
n 51
Sum of
3 harmonics
0.0 0.2 0.4
x/L
(a)
0.6 0.8 1.0
Wave displacement
21
1
0
n 53
n 52
n 51
Sum of
3 harmonics
0.0 0.2 0.4
x/L
(b)
0.6 0.8 1.0
Wave displacement
21
Figure 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 equation
z(x,t)
∑∞
n 1
Ansin
(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 is
z(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).