So, the answer is
The observed frequency when a source emitting frequency is moving towards a stationary observer at speed is given by:
where: - is the speed of sound (assumed to be 330 m/s), - is the speed of the source.
In this case, the sound is reflected off a wall, which acts as a stationary "observer" first. Then, the reflected sound with frequency acts as a source moving towards the driver (now the observer) at speed . So, the frequency heard by the driver is:
where we’ve used since the driver is approaching the wall.
The change in frequency is given as 40 Hz:
Substitute the expression for :
Simplify the equation:
Simplify further:
Given that and , we can solve for :
Simplify:
Solve for :
The frequency of the horn is .
A sub-atomic particle of mass kg is moving with a velocity of m/s. Under the matter wave consideration, the particle will behave closely like (h = J.s)
Waves are a disturbance through which the energy travels from one point to another. Most acquainted are surface waves that tour on the water, but sound, mild, and the movement of subatomic particles all exhibit wavelike properties. inside the most effective waves, the disturbance oscillates periodically (see periodic movement) with a set frequency and wavelength.
Waves in which the medium moves at right angles to the direction of the wave.
Examples of transverse waves:
The high point of a transverse wave is a crest. The low part is a trough.
A longitudinal wave has the movement of the particles in the medium in the same dimension as the direction of movement of the wave.
Examples of longitudinal waves: