To solve this problem, we need to understand the relationship between tension and the speed of a transverse wave on a string. The speed \( v \) of a wave on a string is given by the equation: \( v = \sqrt{\frac{T}{\mu}} \), where \( T \) is the tension in the string and \( \mu \) is the linear mass density of the string.
If the initial tension is \( T_1 \) and the initial speed of the wave is \( v_1 = \sqrt{\frac{T_1}{\mu}} \), then when the tension is doubled, the new tension \( T_2 \) is \( 2T_1 \). The new speed \( v_2 \) is \( v_2 = \sqrt{\frac{2T_1}{\mu}} \).
To find the ratio of the initial and final speeds, we calculate:
\( \frac{v_1}{v_2} = \frac{\sqrt{\frac{T_1}{\mu}}}{\sqrt{\frac{2T_1}{\mu}}} = \frac{\sqrt{T_1}}{\sqrt{2T_1}} = \frac{1}{\sqrt{2}} \).
Thus, the ratio of the initial speed to the final speed is \( 1:\sqrt{2} \).
Initial Speed \(v_1\) | \(\sqrt{\frac{T_1}{\mu}}\) |
Final Speed \(v_2\) | \(\sqrt{\frac{2T_1}{\mu}}\) |
Ratio \(v_1:v_2\) | 1:\(\sqrt{2}\) |
The correct answer is (C) : \(1:\sqrt2\)
Given :
Tension in the string = T,
Mass per unit length = μ,
Velocity of transverse wave on a string , v = \(\sqrt{\frac{\bar{T}}{\mu}}\)
\(v_1=\sqrt{\frac{T_1}{\mu}}\)
\(v_2=\sqrt{\frac{T_2}{\mu}}\)
As per question T2 = 2T1
\(\frac{v_1}{v_2}=\sqrt{\frac{\bar{1}}{2}}=\frac{1}{\sqrt2}\)
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The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
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Examples of transverse waves:
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Examples of longitudinal waves: