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A wave propagates in a string in the pos...

A wave propagates in a string in the positive x-direction with velocity v. The shape of the string at `t=t_0` is given by
`f(x,t_0)=A sin ((x^2)/(a^2))`. Then the wave equation at any instant t is given by

A

`g(x,t)=A sin""[x-v(t-t_0)]^2/(a^2)`

B

`g(x,t)=A sin""[x+v(t-t_0)]^2/(a^2)`

C

`g(x,t)=A sin""[x-v(t+t_0)]^2/(a^2)`

D

`g(x,t)=A sin""[x+v(t+t_0)]^2/(a^2)`

Text Solution

AI Generated Solution

The correct Answer is:
To derive the wave equation for the given scenario, we start with the provided information about the wave shape at a specific time \( t_0 \). ### Step-by-Step Solution: 1. **Identify the Initial Wave Shape**: The shape of the string at time \( t = t_0 \) is given by: \[ f(x, t_0) = A \sin\left(\frac{x^2}{a^2}\right) \] 2. **General Form of Wave Equation**: The general equation for a wave propagating in the positive x-direction is: \[ g(x, t) = A \sin\left(kx - \omega t\right) \] where \( k \) is the wave number and \( \omega \) is the angular frequency. 3. **Relate Wave Parameters**: We know that the wave speed \( v \) is related to the wavelength \( \lambda \) and the period \( T \) by: \[ v = \frac{\lambda}{T} \] From this, we can express \( T \) as: \[ T = \frac{\lambda}{v} \] 4. **Compare Given Wave Shape with General Form**: The given wave shape does not have a time-dependent term. To incorporate time, we consider the wave's propagation from \( t_0 \) to a later time \( t \). We can express the wave at time \( t \) as: \[ g(x, t) = A \sin\left(\frac{x^2}{a^2} - \frac{v}{a}(t - t_0)\right) \] 5. **Substituting the Wave Parameters**: We can rewrite the wave equation using the relationship between \( k \) and \( a \): \[ g(x, t) = A \sin\left(\frac{x^2}{a^2} - \frac{v}{a}(t - t_0)\right) \] 6. **Final Wave Equation**: The final wave equation at any time \( t \) is: \[ g(x, t) = A \sin\left(\frac{x - vt + vt_0}{a}\right) \] This can be simplified to: \[ g(x, t) = A \sin\left(\frac{x - vt + vt_0}{a}\right) \] ### Final Result: Thus, the wave equation at any instant \( t \) is: \[ g(x, t) = A \sin\left(\frac{x - v(t - t_0)}{a}\right) \]
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