Home
Class 12
PHYSICS
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 wave propagating in a string, we start with the shape of the string at a specific time \( t = t_0 \). ### Step-by-Step Solution: 1. **Identify the Given Function**: The shape of the string at time \( t_0 \) is given by: \[ f(x, t_0) = A \sin\left(\frac{x^2}{a^2}\right) \] 2. **Understand the Wave Propagation**: The wave is propagating in the positive x-direction with velocity \( v \). The general form of a wave traveling in the positive x-direction can be expressed as: \[ f(x, t) = A \sin\left(kx - \omega t\right) \] where \( k \) is the wave number and \( \omega \) is the angular frequency. 3. **Relate Time and Position**: At \( t = t_0 \), we want the wave function to match the given function. Thus, we can set: \[ f(x, t_0) = A \sin\left(kx - \omega t_0\right) \] To ensure that this matches the given function, we need: \[ kx - \omega t_0 = \frac{x^2}{a^2} \] 4. **Determine Wave Parameters**: To match the forms, we can equate: \[ k = \frac{2}{a^2} \quad \text{and} \quad \omega t_0 = 0 \quad \text{(since at } t = t_0, \text{ the term must vanish)} \] This implies that \( \omega = 0 \) at \( t = t_0 \), but we need to express the wave function for any time \( t \). 5. **Expressing the Wave Equation**: The wave function can be expressed as: \[ f(x, t) = A \sin\left(kx - \omega t\right) \] Substituting \( k = \frac{2}{a^2} \) and using the relationship between angular frequency and wave speed \( \omega = \frac{2\pi}{T} \) (where \( T \) is the period), we can write: \[ f(x, t) = A \sin\left(\frac{x^2}{a^2} - \frac{v}{a}t\right) \] 6. **Final Form of the Wave Equation**: Therefore, the wave equation at any instant \( t \) is: \[ f(x, t) = A \sin\left(\frac{x^2}{a^2} - \frac{vt}{a}\right) \] ### Final Answer: The wave equation at any instant \( t \) is: \[ f(x, t) = A \sin\left(\frac{x^2}{a^2} - \frac{vt}{a}\right) \]
Promotional Banner

Topper's Solved these Questions

  • PHYSICS PART-III

    FIITJEE|Exercise ASSIGNMENT SECTION-II SUBJECTIVE|27 Videos
  • PHYSICS PART-III

    FIITJEE|Exercise ASSIGNMENT SECTION-II MCQ (SINGLE CORRECT)|47 Videos
  • OPTICS

    FIITJEE|Exercise NUMERICAL BASED QUESTIONS|2 Videos
  • PHYSICS PART2

    FIITJEE|Exercise Numerical Based Question Decimal Type|6 Videos

Similar Questions

Explore conceptually related problems

A wave pulse is travelling on a string with a speed v towards the positive X-axis. The shape of the string at t = 0 is given by g(x) = A sin(x /a) , where A and a are constants. (a) What are the dimensions of A and a ? (b) Write the equation of the wave for a general time 1, if the wave speed is v.

A wave pulse is travelling on a string at 2m//s along positive x-directrion. Displacement y of the particle at x = 0 at any time t is given by y = (2)/(t^(2) + 1) Find Shape of the pulse at t = 0 and t = 1s.

A wave is propagating along x-axis. The displacement of particles of the medium in z-direction at t=0 is given by : z= exp[-(x+2)^(2)] where 'x' is in meter. At t=1s, the same wave disturbance is given by z=exp[-(x-2)^(2)] . Then the wave propagation velocity is :-

A sinusoidal wave having wavelength of 6 m propagates along positive x direction on a string. The displacement (y) of a particle at x = 2 m varies with time (t) as shown in the graph (a) Write the equation of the wave (b) Draw y versus x graph for the wave at t = 0

A sinusoidal wave y=a sin ((2pi)/lambda x-omegat) is travelling on a stretched string. An observer is travelling along positive x direction with a velocity equal to that of the wave. Find the angle that the velocity of a particle on the string at x=lambda/6 makes with -x direction as seen by the observer at time t=0 .

A wave is propagating in positive x- direction. A time t=0 its snapshot is taken as shown. If the wave equation is y=A sin(omegat-Kx+phi) , then phi is