Show that y(x,t)=y1(x,t)+y2(x,t) is a solution to the wave equation

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SUMMARY

The discussion focuses on demonstrating that the function y(x,t) = y1(x,t) + y2(x,t), where y1(x,t) = A cos(k1 x - ω1 t) and y2(x,t) = A cos(k2 x - ω2 t), is a solution to the wave equation ∂²y/∂x² = (1/v²) ∂²y/∂t². Participants confirm that since y1 and y2 are solutions, their sum also satisfies the wave equation due to the principle of superposition. The mathematical manipulation involves applying linearity in differentiation to show that the second derivatives of y1 and y2 combine appropriately to yield the required form.

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  • Understanding of wave equations and their solutions
  • Familiarity with trigonometric identities and calculus
  • Knowledge of the principle of superposition in linear systems
  • Basic understanding of partial derivatives
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  • Learn about the derivation and applications of the wave equation
  • Explore trigonometric identities and their use in solving differential equations
  • Investigate the implications of linearity in differential equations
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Homework Statement


Let y_{1}(x,t)=Acos(k_{1}x-ω_{1}t) and y_{2}(x,t)=Acos(k_{2}-ω_{2}t) be two solutions to the wave equation
\frac{∂^{2}y}{∂x^{2}}=\frac{1}{v^{2}}\frac{∂^{2}y}{∂t^{2}}
for the same v. Show that y(x,t)=y_{1}(x,t)+y_{2}(x,t) is also a solution to the wave equation.

Homework Equations


Equations given in problem statement and

cos(a-b)=cosacosb+sinasinb

The Attempt at a Solution



I am pretty sure I put y_{1}(x,t)+y_{2}(x,t) in a form that does not involve addition like 2Acosasinb or something close to that. Then I take a second partial derivative with respect to both x and t and show that the ratio of ∂^{2}y/∂t^{2} over ∂^{2}2/∂x^{2} is equal to v^{2}.
I am hung up on the trig.

y(x,t)=y_{1}(x,t)+y_{2}(x,t)

y(x,t)=Acos(k_{1}x-ω_{1}t)+Acos(k_{2}-ω_{2}t)

y(x,t)=A(cosk_{1}xcosω_{1}t+sink_{1}xsinω_{1}t)+A(cosk_{2}xcosω_{2}t+sink_{2}xsinω_{2}t)

Cant figure out where to go from here. Please help! Thanks.
 
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You're making it too complicated. Don't use any trig identities. You know that y1 and y2 are solutions. What does that mean mathematically?
 
That their sum should also be a solution by the principle of superposition?
 
Well, that's what you're supposed to show. :wink:

When you assume ##y_i## is a solution, you can say that
$$\frac{\partial^2}{\partial x^2}y_i(x,y) = \frac{1}{v^2}\frac{\partial^2}{\partial t^2} y_i(x,t),$$ where ##\frac{\omega_i}{k_i} = v##.

So now plug ##y=y_1+y_2## into the lefthand side of the wave equation. You get
$$\frac{\partial^2}{\partial x^2}y = \frac{\partial^2}{\partial x^2}(y_1+y_2)$$ which you can split into two terms because differentiation is a linear operation. What you want to do is keep manipulating the righthand side until you end up with
$$\frac{1}{v^2} \frac{\partial^2}{\partial t^2}y.$$
 
\frac{\partial^2}{\partial x^2}y = \frac{\partial^2}{\partial x^2}(y_1+y_2)
\frac{\partial^2}{\partial x^2}y = \frac{\partial^2 y_1}{\partial x^2} + \frac{\partial^2 y_2}{\partial x^2}
\frac{\partial^2}{\partial x^2}y = \frac{1}{v^2}\frac{\partial^2 y_1}{\partial t^2}+\frac{1}{v^2}\frac{\partial^2 y_1}{\partial t^2}
\frac{\partial^2}{\partial x^2}y = \frac{1}{v^2}(\frac{\partial^2 y_1}{\partial t^2}+\frac{\partial^2 y_2}{\partial t^2})
\frac{\partial^2}{\partial x^2}y= \frac{1}{v^2}\frac{\partial^2}{\partial t^2}(y_1+y_2)
\frac{\partial^2}{\partial x^2}y = \frac{1}{v^2}\frac{\partial^2}{\partial t^2}y

Is that all I have to show since I already know that y is a solution to the wave equation and that it is assumed that is obeys that principle of superposition? Thanks again for your time.
 

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