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The time period of a physical pendulum i...

The time period of a physical pendulum is given by `T=2pisqrt(I/(mgl))`. Where m= mass of the pendulum I= moment of inertia about the axis of suspension, l= distance of centre of mass of bob from the centre of suspension. Calculate the change in time period when temperature changes by `DeltaT`. The coefficient of linear expansion of the material of pendulum is `alpha`.

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To calculate the change in the time period of a physical pendulum when the temperature changes by \(\Delta T\), we will follow these steps: ### Step 1: Understand the Formula for Time Period The time period \(T\) of a physical pendulum is given by: \[ T = 2\pi \sqrt{\frac{I}{mgl}} \] where: - \(I\) = moment of inertia about the axis of suspension - \(m\) = mass of the pendulum - \(g\) = acceleration due to gravity - \(l\) = distance from the center of mass to the center of suspension ### Step 2: Determine the Effect of Temperature Change When the temperature changes by \(\Delta T\), the dimensions of the pendulum will change due to thermal expansion. The linear expansion of a material is given by: \[ L' = L(1 + \alpha \Delta T) \] where: - \(L\) = original length - \(\alpha\) = coefficient of linear expansion - \(L'\) = new length after expansion ### Step 3: Calculate the New Moment of Inertia The moment of inertia \(I\) for a pendulum can be expressed as: \[ I = mL^2 \] After the temperature change, the new moment of inertia \(I'\) becomes: \[ I' = m(L')^2 = m[L(1 + \alpha \Delta T)]^2 = mL^2(1 + \alpha \Delta T)^2 \] ### Step 4: Calculate the New Length from the Center of Suspension The new length \(l'\) from the center of suspension is also affected by the temperature change: \[ l' = l(1 + \alpha \Delta T) \] ### Step 5: Substitute New Values into the Time Period Formula The new time period \(T'\) can be expressed as: \[ T' = 2\pi \sqrt{\frac{I'}{mg l'}} = 2\pi \sqrt{\frac{mL^2(1 + \alpha \Delta T)^2}{mg l(1 + \alpha \Delta T)}} \] Simplifying this gives: \[ T' = 2\pi \sqrt{\frac{L^2(1 + \alpha \Delta T)^2}{gl(1 + \alpha \Delta T)}} \] This can be further simplified to: \[ T' = 2\pi \sqrt{\frac{L^2}{gl}}(1 + \alpha \Delta T)^{1/2} \] ### Step 6: Relate New Time Period to Original Time Period We know that: \[ T = 2\pi \sqrt{\frac{L^2}{gl}} \] Thus, we can write: \[ T' = T(1 + \alpha \Delta T)^{1/2} \] ### Step 7: Calculate the Change in Time Period The change in time period \(\Delta T\) is given by: \[ \Delta T = T' - T = T(1 + \alpha \Delta T)^{1/2} - T \] Using the binomial expansion for small \(\alpha \Delta T\): \[ (1 + x)^{1/2} \approx 1 + \frac{x}{2} \text{ for small } x \] we can approximate: \[ \Delta T \approx T\left(\frac{\alpha \Delta T}{2}\right) = \frac{T \alpha \Delta T}{2} \] ### Final Result Thus, the change in time period when the temperature changes by \(\Delta T\) is: \[ \Delta T \approx \frac{T \alpha \Delta T}{2} \]
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PHYSICS GALAXY - ASHISH ARORA-HEAT AND THERMAL EXPANSION-PRACTICE EXERCISE
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