Animated Solution for Physics - Waves: A wire of length L and mass per unit length 6.0×10−3 kgm−1 is put under tension of 540 N. Two consecutive frequencies that it resonates at are : 420 Hz and 490 Hz. Then, L in metres is
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Visualized Solution
\text{The Stretched String}
A wire of length L is stretched under tension T.
\text{Resonant Frequencies}
The n-th resonant frequency is given by:
fn=2LnμT
\text{Consecutive Frequencies}
Let the two consecutive frequencies be fn and fn+1.
fn=2LnμT=420 Hz
fn+1=2Ln+1μT=490 Hz
\text{Fundamental Frequency}
Subtracting the two equations:
fn+1−fn=2L1μT
490−420=70 Hz
\text{Solving for } L
2L16.0×10−3540=70
2L190000=70
2L300=70
\text{Final Length}
L=2×70300=140300
L≈2.14 m
\text{What if?}
How would the resonant frequencies change if the tension in the wire is doubled?
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The Sigma Insight: Standing Waves in Strings and Organ Pipes
Solution Diagram
Understanding the Physics of Stretched Strings
Imagine a guitar string pulled tightly between two fixed points. When you pluck it, the string vibrates, creating a beautiful standing wave. The frequencies at which this string naturally wants to vibrate are called its resonant frequencies or harmonics.
For a string of length L, fixed at both ends, the resonant frequencies are not just random numbers. They follow a strict, elegant mathematical rule. The n-th resonant frequency is given by the formula:
fn=2LnμT
Here, T is the tension in the string, μ is the linear mass density (mass per unit length), and n is an integer (1,2,3,…) representing the harmonic number. The fundamental frequency, or the first harmonic, occurs when n=1.
The Magic of Consecutive Harmonics
In our problem, we are given two consecutive resonant frequencies: 420 Hz and 490 Hz. Because they are consecutive, if the first one is the n-th harmonic, the next one must be the (n+1)-th harmonic.
Let's write down the equations for these two frequencies:
fn=2LnμT=420 Hz
fn+1=2Ln+1μT=490 Hz
Now, here is where the magic happens. If we subtract the n-th frequency from the (n+1)-th frequency, the terms involving n completely cancel out!
fn+1−fn=(2Ln+1−2Ln)μT=2L1μT
Notice that the result is exactly the formula for the fundamental frequency (f1). This is a powerful shortcut: The difference between any two consecutive harmonic frequencies of a string fixed at both ends is always equal to its fundamental frequency.
So, we can easily find the fundamental frequency:
f1=490 Hz−420 Hz=70 Hz
Crunching the Numbers
Now that we know the fundamental frequency is 70 Hz, we can use it to find the length of the string L. We are given the tension T=540 N and the linear mass density μ=6.0×10−3 kg/m.
Let's plug these values into our fundamental frequency equation:
2L16.0×10−3540=70
First, let's simplify the term inside the square root. Dividing 540 by 6.0×10−3 is the same as 540×61000, which gives 90000.
2L190000=70
The square root of 90000 is exactly 300. So our equation simplifies beautifully to:
2L300=70
Now, it's just a matter of simple algebra to isolate L:
2L=70300
L=140300=715
Calculating the decimal value, we get:
L≈2.1428 m
Looking at the options provided in the question, the closest value is 2.1 m. Thus, the correct option is (b).