Let us assume that the wave pulse created during this disturbance moves along positive x direction with constant speed v.

Equation of a plane progressive wave

Suppose we give a jerk on a stretched string at time *t* = 0*s*. Let us assume that the wave pulse created during this disturbance moves along positive *x* direction with constant speed *v* as shown in Figure 11.23 (a). We can represent the shape of the wave pulse, mathematically as *y* = *y*(*x*, 0) = *f*(*x*) at time *t* = 0*s*. Assume that the shape of the wave pulse remains the same during the propagation. After some time *t*, the pulse moving towards the right and any point on it can be represented by *x*' (read it as *x *prime) as shown in Figure 11.23 (b). Then,

Similarly, if the wave pulse moves towards left with constant speed *v*, then *y* = *f*(*x* + *vt*). Both waves *y* = *f*(*x* + *vt*) and *y* = *f*(*x* âˆ’ *vt*) will satisfy the following one dimensional differential equation known as the wave equation

where the symbol âˆ‚ represent partial (read âˆ‚y/âˆ‚x as partial y by partial x). Not all the solutions satisfying this differential equation can represent waves, because any physical acceptable wave must take finite values for all values of x and t. But if the function represents a wave then it must satisfy the differential equation. Since, in one dimension (one independent variable), the partial derivative with respect to x is the same as total derivative in coordinate x, we write

This can be extended to more than one dimension (two, three, etc.). Here, for simplicity, we focus only on the one dimensional wave equation.

Sketch *y* = *x* âˆ’*a* for different values of *a*.

This implies, when increasing the value of *a*, the line shifts towards right side. For *a *=* vt*,* y *=* x *âˆ’* vt *satisfies the differential* *equation. Though this function satisfies the differential equation, it is not finite for all values of *x* and *t*. Hence, it does not represent a wave.

How does the wave *y* = sin(*x* âˆ’ *a*) for *a* = 0, a = Ï€/4, a = Ï€/2, a = 3Ï€/2, a = Ï€ look like?. Sketch this wave.

From the above picture we observe that *y = sin (xâˆ’a) for a = 0, a = Ï€/4, a = Ï€/2, a = 3Ï€/2 and a = Ï€, the function y = sin (xâˆ’a) *shifts towards right. Further, we can take* *a = vt and v = Ï€/4 , and sketching for different times *t* = 0*s*, *t* = 1 *s*, *t* = 2*s* etc., we once again observe that *y* = sin(*x*âˆ’*vt*) moves towards the right. Hence, *y* = sin(*x*âˆ’*vt*) is a travelling (or progressive) wave moving towards the right. If *y* = sin(*x*+*vt*) then the travelling (or progressive) wave moves towards the left. Thus, any arbitrary function of type *y *=* f*(*x*âˆ’*vt*) characterising the wave must* *move towards right and similarly, any arbitrary function of type *y* = *f*(*x*+*vt*) characterizing the wave must move towards left.

Check the dimensional of the wave *y* = sin(*x*âˆ’*vt*). If it is dimensionally wrong, write the above equation in the correct form.

Dimensionally it is not correct. we know that *y* = sin(*x*âˆ’*vt*) must be a dimensionless quantity but *x*âˆ’*vt* has dimension. The correct equation is *y* = sin (*k x*âˆ’*Ï‰t*), where *k *and* Ï‰ *have the dimensions of inverse* *of length and inverse of time respectively. The sine functions and cosine functions are periodic functions with period 2Ï€. Therefore, the correct expression is y = sin ([2Ï€/Î»]x, [2Ï€/T]t) where Î» and T are wavelength and time period, respectively.

In general, *y*(*x*,*t*)=A sin(*k x*âˆ’*Ï‰t*).

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11th Physics : UNIT 11 : Waves : Equation of a plane progressive wave (or) Travelling Wave |

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