For an open organ pipe, the harmonics produced are integer multiples of the fundamental frequency. For a closed organ pipe, only odd harmonics are produced.
Let's analyze the situation step by step:
The frequency of the nth harmonic for an open pipe is given by:
\(f_n = n \times \frac{v}{2L_{\text{open}}}\)
For the second overtone of the open pipe, this corresponds to the third harmonic:
\(f_3 = 3 \times \frac{v}{2L_{\text{open}}}\)
The frequency of the nth harmonic for a closed pipe is given by:
\(f_n = n \times \frac{v}{4L_{\text{closed}}}\)
For the first overtone of the closed pipe, this corresponds to the third harmonic:
\(f_1 = \frac{v}{4L_{\text{closed}}}\)
Since both frequencies are equal, we equate them:
\(3 \times \frac{v}{2L_{\text{open}}} = \frac{v}{4L_{\text{closed}}}\)
Canceling out \(v\) from both sides:
\(3 \times \frac{1}{2L_{\text{open}}} = \frac{1}{4L_{\text{closed}}}\)
Cross-multiplying gives:
\(12L_{\text{closed}} = 2L_{\text{open}}\)
Dividing both sides by 2:
\(6L_{\text{closed}} = L_{\text{open}}\)
The length of the open pipe is \(L_{\text{open}} = 6L_{\text{closed}}\).
Therefore, the correct answer is 2L.
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: