A plane progressive wave is typically represented by equations involving sinusoidal functions of time and space.
A. \(y = a \sin(\omega t \pm kx)\):
This is a standard form representing a plane progressive wave, where \(\omega\) is the angular frequency, k is the wave number, t is time, and x is position.
B. \(y = a \sin \left( 2\pi \left( \frac{t}{T} \mp \frac{x}{\lambda} \right) \right)\):
This is also a valid representation of a plane progressive wave, where T is the period and \(\lambda\) is the wavelength.
C. \(y = a \sin \left( \frac{2\pi}{\lambda} (Vt \mp x) \right)\):
This is another valid form, where V represents the wave velocity, t is time, and x is position.
D. \(y = A \log x + B \log x\):
This equation is not a typical representation of a plane progressive wave. It involves logarithmic functions of x, which do not describe the oscillatory nature of a wave propagating through space and time.
So, the correct answer is (D): \(y = A \log x + B \log x\).
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: