Maximum transverse velocity of a wave along a string

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SUMMARY

The maximum transverse velocity of a wave along a string with fixed ends, traveling at a speed of 40 m/s, can be calculated using the wave equation y = A Sin(kx - wt). The wave has a wavelength of 2 meters, leading to a wave number of π and a frequency of 20 Hz, resulting in an angular frequency of 40π. The maximum transverse velocity is derived from the derivative of the wave function, yielding a maximum value of 12.5 m/s, which contradicts the textbook answer of 4 m/s. This discrepancy arises from the nature of the wave pulse, which is not sinusoidal and requires the use of the slope of the wave pulse for accurate calculations.

PREREQUISITES
  • Understanding of wave equations, specifically y = A Sin(kx - wt)
  • Knowledge of wave properties such as wavelength, frequency, and angular frequency
  • Familiarity with calculus, particularly derivatives and their application in physics
  • Concept of wave pulses and their representation in mathematical terms
NEXT STEPS
  • Study the derivation of wave equations and their applications in different wave types
  • Learn about the relationship between wave speed, frequency, and wavelength in more detail
  • Explore the concept of wave pulse versus sinusoidal waves and their mathematical representations
  • Investigate the use of partial derivatives in analyzing wave motion and velocity
USEFUL FOR

Students studying physics, particularly those focusing on wave mechanics, as well as educators and anyone involved in teaching or learning about wave behavior in strings.

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Homework Statement



The figure (attached image) shows a pulse on a string of length 100m with fixed ends. The pulse is traveling to the right without any change of shape, at a speed of 40 m/s.

What is the maximum transverse velocity of the string?

Homework Equations



y = A Sin(kx-wt)

The Attempt at a Solution



I said that the wave had a length of 2 meters. That makes the wave number 2pi/2 = pi. And since we know the velocity and wavelength, we can find the frequency, and therefore, the angular frequency. 40(m/s)/2m = 20 hz. w=2 pi f = 2 pi 20 = 40 pi. And the amplitude is .1 m.

This makes the equation y = .1 Sin(pi x - 40 pi t)

The velocity is the derivative of position, giving us -12.5 Cos[40 pi t - pi x].

Therefore, the maximum velocity would be when the derivative of velocity = 0.
y''=a= 1580 Sin[40 pi t - pi x].

I get that y'' = 0 when either x=40t or t=x/40. If I plug this into y', I get the argument in the cosine to equal 0, which makes cosine equal 1. This would just leave the constant term as the answer, making it (a magnitude of) 12.5 m/s. But according to the book, the answer is 4 m/s. How did they get this?
 

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The graph shows a wave pulse, not a sinusoidal wave. The wave pulse would be represented by some function of the form ##y(x, t) = f(x-vt)##, where ##v## is the wave speed. It will be useful to think of this as

##y(x, t) = f(u)##, where ##u \equiv x - vt##

Note that at any fixed time ##t##, the slope of the wave pulse at position ##x## is given by

slope = ##\frac{\partial y}{\partial x} = \frac{\partial f}{\partial u} \frac{\partial u}{\partial x}##.

Since ##\frac{\partial u}{\partial x} = 1##, we have slope = ##\frac{\partial f}{\partial u}##

Similarly, the vertical velocity ##V_y## of a point of the string at position ##x## is given by

##V_y = \frac{\partial y}{\partial t} = \frac{\partial f}{\partial u}\frac{\partial u}{\partial t}##.

Since ##\frac{\partial u}{\partial t} = -v##, we have ## V_y = -v \frac{\partial f}{\partial u}##.

Or, since ##\frac{\partial f}{\partial u} = ## slope, ## V_y = -v \cdot slope##.

You can use this to help sketch the graph of ## V_y## as a function of ##x## for the time shown in the figure.

To estimate the maximum value of ## V_y \,##, use the figure to estimate the maximum slope of the wave pulse.
 
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