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Show that the equation,y=a sin(omegat-kx...

Show that the equation,`y=a sin(omegat-kx)` satisfies the wave equation`(del^(2) y)/(delt^(2))=v^(2) (del^(2)y)/(delx^(2))`. Find speed of wave and the direction in which it is travelling.

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To show that the equation \( y = a \sin(\omega t - kx) \) satisfies the wave equation \[ \frac{\partial^2 y}{\partial t^2} = v^2 \frac{\partial^2 y}{\partial x^2}, \] we will follow these steps: ### Step 1: Differentiate \( y \) with respect to \( t \) Given: \[ y = a \sin(\omega t - kx) \] We first find the first derivative of \( y \) with respect to \( t \): \[ \frac{\partial y}{\partial t} = a \omega \cos(\omega t - kx) \] ### Step 2: Differentiate again with respect to \( t \) Now, we differentiate \( \frac{\partial y}{\partial t} \) again with respect to \( t \): \[ \frac{\partial^2 y}{\partial t^2} = -a \omega^2 \sin(\omega t - kx) \] ### Step 3: Differentiate \( y \) with respect to \( x \) Next, we find the first derivative of \( y \) with respect to \( x \): \[ \frac{\partial y}{\partial x} = -a k \cos(\omega t - kx) \] ### Step 4: Differentiate again with respect to \( x \) Now, we differentiate \( \frac{\partial y}{\partial x} \) again with respect to \( x \): \[ \frac{\partial^2 y}{\partial x^2} = -a k^2 \sin(\omega t - kx) \] ### Step 5: Substitute into the wave equation Now we substitute \( \frac{\partial^2 y}{\partial t^2} \) and \( \frac{\partial^2 y}{\partial x^2} \) into the wave equation: \[ -a \omega^2 \sin(\omega t - kx) = v^2 (-a k^2 \sin(\omega t - kx)) \] ### Step 6: Simplify the equation We can simplify this equation by dividing both sides by \( -a \sin(\omega t - kx) \) (assuming \( a \neq 0 \) and \( \sin(\omega t - kx) \neq 0 \)): \[ \omega^2 = v^2 k^2 \] ### Step 7: Solve for \( v \) From the equation \( \omega^2 = v^2 k^2 \), we can solve for \( v \): \[ v^2 = \frac{\omega^2}{k^2} \] Taking the square root of both sides, we find: \[ v = \frac{\omega}{k} \] ### Step 8: Determine the direction of the wave The wave function \( y = a \sin(\omega t - kx) \) indicates that the wave is traveling in the positive x-direction because of the negative sign in front of \( kx \). ### Summary of Results - The speed of the wave is given by \( v = \frac{\omega}{k} \). - The wave is traveling in the positive x-direction.

To show that the equation \( y = a \sin(\omega t - kx) \) satisfies the wave equation \[ \frac{\partial^2 y}{\partial t^2} = v^2 \frac{\partial^2 y}{\partial x^2}, \] we will follow these steps: ...
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