In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:

Step 1: Understanding Wave Speed in a Stretched String The speed of a transverse wave in a stretched string is given by: \[ v = \sqrt{\frac{T}{\mu}} \] where: \( T \) is the tension in the string, \( \mu \) is the mass per unit length. Since both strings are made of the same material and have the same cross-section, their linear mass densities (\(\mu\)) are equal.
Step 2: Analyzing Tension in the Strings - Let the tension in string AB be \( T_1 \). - The tension in string CD, which supports an additional load due to the pulley arrangement, is given by: \[ T_2 = 2T_1 \]
Step 3: Finding the Velocity Ratio Using the wave speed formula: \[ v_1 = \sqrt{\frac{T_1}{\mu}}, \quad v_2 = \sqrt{\frac{T_2}{\mu}} \] \[ v_2 = \sqrt{\frac{2T_1}{\mu}} = \sqrt{2} v_1 \] Thus, the ratio is: \[ \frac{v_1}{v_2} = \frac{v_1}{\sqrt{2} v_1} = \frac{1}{\sqrt{2}} \]
Three point particles of masses 1.0 kg, 1.5 kg and 2.5 kg are placed at three corners of a right-angle triangle of sides 4.0 cm, 3.0 cm and 5.0 cm as shown in the figure. The center of mass of the system is at a point:
In the following circuit diagram, when the \(3\Omega\) resistor is removed, the equivalent resistance of the network:

A particle is moving in a straight line. The variation of position $ x $ as a function of time $ t $ is given as:
$ x = t^3 - 6t^2 + 20t + 15 $.
The velocity of the body when its acceleration becomes zero is:
A plane progressive wave is given by y = 2 cos 2pi (330t - x) m. The frequency of the wave is:}
Three point particles of masses 1.0 kg, 1.5 kg and 2.5 kg are placed at three corners of a right-angle triangle of sides 4.0 cm, 3.0 cm and 5.0 cm as shown in the figure. The center of mass of the system is at a point: