Waves

A string is stretched between fixed points separated by 75 75 cm. It is observed to have resonant frequencies of 420 420 Hz and 315 315 Hz. There are no other resonant frequencies between these two. Then, the lowest resonant frequency for this string is _ _.


This question is a part of the set JEE Physics .


The answer is 105.

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2 solutions

Let the velocity of the wave in the string be given by v v , and let the length of the string be given by L L . The wave in a string is formed by both it's ends as nodes. It can be easily seen that, the wavelength, λ \lambda , of the wave formed is given by λ n = 2 L n {\lambda}_{n} = \frac {2L} {n} , where n n is a natural number.

Now, according to the given question, since there is no other frequency between 420 H z 420 Hz and 315 H z 315 Hz , hence these frequencies can be written as

ν n = v λ n = 420 H z {\nu}_{n} = \frac {v} { {\lambda}_{n} } =420 Hz

and ν n 1 = v λ n 1 = 315 H z {\nu}_{n-1} = \frac {v} { {\lambda}_{n-1} } =315 Hz

So, v n 2 L = 420 \frac {v n} {2L} =420 and v ( n 1 ) 2 L = 315 \frac {v (n-1)} {2L} = 315

Solving, the equations, we get n = 4 n=4

Now, the fundamental frequency for a string is given by v 2 L \frac {v} {2L} which can be calculated by using the value of n n .

So, solving the formed equations: v 2 L = 105 H z \frac {v} {2L} = 105 Hz

Duncan McCormick
Jun 25, 2020

This explanation is written in a way which will (hopefully) be useful for those studying A-Level Physics.

From earlier study of harmonics on stationary waves, we know that the first harmonic frequency is f 1 f_{1} = c λ 1 \frac{c}{λ_{1}} , where c c is the wavespeed on the string. We do not need the value of c c to solve this question, but for reference, it can be calculated as T μ 0.5 \frac{T}{μ} ^{0.5} , where T T is the tension in the string, and μ μ is the mass per unit length in the string. The frequency of the first harmonic f 1 f_{1} can be calculated as f 1 = c 2 L f_{1} = \frac{c}{2L} , where L L is the length of the string, because 2 L = λ 1 2L = λ_{1} . You can visualise this by looking at a stationary wave at the first harmonic: there is one "loop" (equal to half a wavelength) between the two fixed ends, meaning that the wavelength λ 1 λ_{1} is twice the distance between the ends of the string.

For the second harmonic frequency, f 2 f_{2} , there are two "loops" between the ends of the string, or one wavelength. Therefore, f 2 f_{2} = c L \frac{c}{L} , as f 2 f_{2} = c λ 2 \frac{c}{λ_{2}} . Rearranging shows that f 2 = 2 f 1 f_{2} = 2f_{1} . It turns out that for the nth harmonic stationary wave, the frequency f n = n f 1 f_{n} = nf_{1} .

We will take the frequency f n = 315 f_{n} = 315 Hz. It is given that there are no harmonics (resonant freqencies) between the two frequencies in the question, so it follows that f n + 1 = 420 f_{n+1} = 420 Hz. Therefore: n f 1 = 315 nf_{1} = 315 ( n + 1 ) f 1 = 420 (n+1)f_{1} = 420 n f 1 + f 1 = 420 nf_{1} + f_{1} = 420 f 1 = 420 315 = 105 f_{1} = 420 - 315 = 105 f 1 = 105 f_{1} = 105 Hz

So the first harmonic (lowest resonant frequency) is 105 Hertz. (Note that we were able to calculate this without taking into account the length of the string)

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