A wave travelling along the $x- $ axis is described by the equation $y(x, t) = 0.005\,\,cos(\alpha x\,-\,\beta t).$ If the wavelength and the time period of the wave are $0.08 \,\,m$ and $2.0\,\,s,$ respectively, then $\alpha $ and $\beta $ in appropriate units are
$\alpha \,\, = \,25.00\,\pi \,\, ;\,\,\beta \, = \,\pi $
$\alpha \,\, = \frac{{0.08}}{\pi }\,\, ;\,\,\beta \, = \,\frac{{2.0}}{\pi }$
$\alpha \,\, = \frac{{0.04}}{\pi }\,\, ;\,\,\beta \, = \,\frac{{1.0}}{\pi }$
$\alpha \,\, = 12.50\pi \,\, ;\,\,\beta \, = \,\frac{\pi }{{2.0}}$
A string of mass $M$ and length $L$ hangs freely from a fixed point. The velocity of transverse wave along the string at a distance $'x'$ from the free end will be
A string of mass $2.5\, kg$ under some tension. The length of the stretched string is $20\, m$. If the transverse jerk produced at one end of the string takes $0.5\, s$ to reach the other end, tension in the string is .... $N$
A closed organ pipe has a frequency $'n'$. If its length is doubled and radius is halved, its frequency nearly becomes
Two waves of sound having intensities $I$ and $4I$ interfere to produce interference pattern. The phase difference between the waves is $\pi /2$ at point $A$ and $\pi$ at point $B$. Then the difference between the resultant intensities at $A$ and $B$ is
Two vibrating strings of the same material but lengths $L$ and $2L$ have radii $2r$ and $r$ respectively. They are stretched under the same tension . Both the strings vibrate in their fundamental modes, the one of length $L$ with frequency $f_1$ and the other with frequency $f_2$. The ratio $\frac{f_1}{f_2}$ is given by