To understand the problem, we need to analyze how the fundamental frequencies of open and closed pipes relate. An open pipe resonates at a fundamental frequency \( f_{\text{open}} \) given by:
\( f_{\text{open}} = \frac{v}{2L} \)
where \( v \) is the speed of sound in air and \( L \) is the length of the pipe.
For a closed pipe (open at one end and closed at the other), the fundamental frequency \( f_{\text{closed}} \) is:
\( f_{\text{closed}} = \frac{v}{4L} \)
Comparing these two equations, the ratio of the fundamental frequencies is:
\(\frac{f_{\text{open}}}{f_{\text{closed}}} = \frac{\frac{v}{2L}}{\frac{v}{4L}} = \frac{4L}{2L} = 2\)
Thus, the ratio of the frequencies of the fundamental harmonic produced by an open pipe to that of a closed pipe of the same length is 2:1.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
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: