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Speed of transverse wave on a string is considered one of the most asked concept.
23 Questions around this concept.
When temperature increases, the frequency of a tuning fork
The distance between two successive crests is 1 wavelength, $\lambda$. Thus in one time period, the wave will travel 1 wavelength in distance. Thus the speed of the wave, v is:
$
v=\frac{\lambda}{T}=\frac{\text { Distance travelled }}{\text { time taken }}
$
The speed of the traverse wave is determined by the restoring force set up in the medium when it is disturbed and the inertial properties ( mass density ) of the medium. The inertial property will in this case be linear mass density $\mu$.
$\mu=\frac{m}{L}$ where m is the mass of the string and L is length.
The dimension of $\mu_{\text {is }}\left[M L^{-1}\right]$ and T is like force whose dimension is $\left[M L T^{-2}\right]$. We need to combine these dimension to get the dimension of speed v which is $\left[L T^{-1}\right]$.
Therefore speed of wave in a string is given as :
$
v=\sqrt{\frac{T}{\mu}}
$
Now Let's understand its derivation.
Take a small element of length dl and mass dm of string as shown in the below figure (a)
Here $d l=R(2 \theta)$
So For figure (b)
$
\frac{d m \times v^2}{R}=2 T \sin \theta
$
For small $\theta$ we can use $\operatorname{Sin} \theta=\theta$
$
\begin{aligned}
& \Rightarrow \frac{d m v^2}{R}=2 T \theta=T \frac{d l}{R} \\
& V^2=\frac{T}{d m / d l}
\end{aligned}
$
Now using
$
\mu=\frac{d m}{d l}
$
we get
$
\Rightarrow V=\sqrt{\frac{T}{\mu}}
$
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