355199 Assertion :
A standing wave pattern is formed in a string. The power transfer through a point (other than node and antinode) is zero always.
Reason :
At antinode displacement is maximum

355200 The equation for the vibration of a string fixed at both ends vibrating in its third harmonic is given by \(y = 2\;cm\sin \left[ {\left( {0.6\;c{m^{ - 1}}} \right)x} \right]\cos \left[ {\left( {500\pi {s^{ - 1}}} \right)t} \right]\) The length of the string is

355201 The length of the wire shown in Fig. between the pulley and fixed support is \(1.5\;m\) and mass is \(12.0\;g\) the frequency of vibration with which the wire vibrate in two loops leaving the middle point of the wire between the pulleys at rest is:

355202 Superposition of two waves \(y_{1}=A \sin (\omega t-k x)\) and \(y_{2}=-A \sin (\omega t+k x)\) gives \(a\) :

355199 Assertion :
A standing wave pattern is formed in a string. The power transfer through a point (other than node and antinode) is zero always.
Reason :
At antinode displacement is maximum

355200 The equation for the vibration of a string fixed at both ends vibrating in its third harmonic is given by \(y = 2\;cm\sin \left[ {\left( {0.6\;c{m^{ - 1}}} \right)x} \right]\cos \left[ {\left( {500\pi {s^{ - 1}}} \right)t} \right]\) The length of the string is

355201 The length of the wire shown in Fig. between the pulley and fixed support is \(1.5\;m\) and mass is \(12.0\;g\) the frequency of vibration with which the wire vibrate in two loops leaving the middle point of the wire between the pulleys at rest is:

355202 Superposition of two waves \(y_{1}=A \sin (\omega t-k x)\) and \(y_{2}=-A \sin (\omega t+k x)\) gives \(a\) :

355199 Assertion :
A standing wave pattern is formed in a string. The power transfer through a point (other than node and antinode) is zero always.
Reason :
At antinode displacement is maximum

355200 The equation for the vibration of a string fixed at both ends vibrating in its third harmonic is given by \(y = 2\;cm\sin \left[ {\left( {0.6\;c{m^{ - 1}}} \right)x} \right]\cos \left[ {\left( {500\pi {s^{ - 1}}} \right)t} \right]\) The length of the string is

355201 The length of the wire shown in Fig. between the pulley and fixed support is \(1.5\;m\) and mass is \(12.0\;g\) the frequency of vibration with which the wire vibrate in two loops leaving the middle point of the wire between the pulleys at rest is:

355202 Superposition of two waves \(y_{1}=A \sin (\omega t-k x)\) and \(y_{2}=-A \sin (\omega t+k x)\) gives \(a\) :

355199 Assertion :
A standing wave pattern is formed in a string. The power transfer through a point (other than node and antinode) is zero always.
Reason :
At antinode displacement is maximum

355200 The equation for the vibration of a string fixed at both ends vibrating in its third harmonic is given by \(y = 2\;cm\sin \left[ {\left( {0.6\;c{m^{ - 1}}} \right)x} \right]\cos \left[ {\left( {500\pi {s^{ - 1}}} \right)t} \right]\) The length of the string is

355201 The length of the wire shown in Fig. between the pulley and fixed support is \(1.5\;m\) and mass is \(12.0\;g\) the frequency of vibration with which the wire vibrate in two loops leaving the middle point of the wire between the pulleys at rest is:

355202 Superposition of two waves \(y_{1}=A \sin (\omega t-k x)\) and \(y_{2}=-A \sin (\omega t+k x)\) gives \(a\) :