Explain the reflection of wave at rigid support.
A pulse (wave) moving in $+x$-direction and reflecting wave from fixed support are shown in
figure.
If we suppose that the energy is not absorbed at end, then the shape of the reflected pulse will be
same as incident but the phase will be changed by $180^{\circ}(\pi)$.
The reason behind it is the end is fixed. So that the displacement of pulse should be zero.
Suppose, the incident progressive wave displacement at ' $t$ ' time is $y_{i}(x, t)=a \sin (k x-\omega t)$.
Suppose, the displacement of reflected wave is $y_{r}$
According to superposition principle,
$y(x, t)=y_{i}(x, t)+y_{r}(x, t)$
But $y(x, t)=0$
$(\because$ displacement of fixed end is zero $)$
$\therefore 0=y_{i}(x, t)+y_{r}(x, t)$
$\therefore y_{r}(x, t)=-y_{i}(x, t)$
$\therefore y_{r}(x, t)=-a \sin (k x-\omega t)$
A vibrating string of certain length $\ell$ under a tension $\mathrm{T}$ resonates with a mode corresponding to the first overtone (third harmonic) of an air column of length $75 \mathrm{~cm}$ inside a tube closed at one end. The string also generates $4$ beats per second when excited along with a tuning fork of frequency $\mathrm{n}$. Now when the tension of the string is slightly increased the number of beats reduces $2$ per second. Assuming the velocity of sound in air to be $340 \mathrm{~m} / \mathrm{s}$, the frequency $\mathrm{n}$ of the tuning fork in $\mathrm{Hz}$ is
A string is stretched between fixed points separated by $75.0\, cm$. It is observed to have resonant frequencies of $420\, Hz$ and $315\, Hz$. There are no other resonant frequencies between these two. Then, the lowest resonant frequency for this string is .... $Hz$
In an experiment with sonometer a tuning fork of frequency $256 Hz$ resonates with a length of $25 cm$ and another tuning fork resonates with a length of $16 cm$. Tension of the string remaining constant the frequency of the second tuning fork is .... $Hz$
A $12 \,m$ long vibrating string has the speed of wave $48 \,m / s$. To what frequency it will resonate ........... $cps$
A second harmonic has to be generated in a string of length $l$ stretched between two rigid supports. The point where the string has to be plucked and touched are