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16.2 Exercise 2

Avg difficulty 2.5

The wave equation ∂2y(x,t)∂x2=1v2∂2y(x,t)∂t2\frac{\partial^{2} y \left(x , t\right)}{\partial x^{2}} = \frac{1}{v^{2}} \frac{\partial^{2} y \left(x , t\right)}{\partial t^{2}} works for any wave of the form y(x,t)=f(x∓vt).y \left(x , t\right) = f \left(x +- v t\right) . In the previous section, we stated that a cosine function could also be used to model a simple harmonic mechanical wave. Check if the wave

y(x,t)=0.50mcos(0.20πm−1x−4.00πs−1t+π10)y \left(x , t\right) = 0.50 \text{m} \text{cos} \left(0.20 \pi \text{m}^{−1} x - 4.00 \pi \text{s}^{−1} t + \frac{\pi}{10}\right)

is a solution to the wave equation.

OpenStax University Physics Volume 1, 16.2 Mathematics of Waves, exercise 2

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Adapted from University Physics Volume 1 © 2016 Rice University. Licensed under CC BY 4.0. Source: University Physics Volume 1. Imported at revision db44eb9.