Flag Wave Motion> Figure shows a physical pendulum construc...
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Figure shows a physical pendulum constructed from equal-length sections of identical pipe. The inner radius of the pipe is 10.2 cm and the thickness is 6.40 mm.
(a) Calculate the period of oscillation about the pivot shown.
(b) Suppose that a new physical pendulum is constructed by rotating the bottom section 90° about a vertical axis through its center. Show that the new period of oscillation about the same pivot is about 2% less than the period of the original pendulum.
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

Simran Bhatia , 10 Years ago
Grade 11
anser 1 Answers
Askiitians Tutor Team

To tackle the problem of calculating the period of oscillation for the physical pendulum and understanding the effects of modifying its structure, we need to delve into some fundamental concepts of physics, particularly those related to rotational motion and pendulum dynamics. Let's break this down step by step.

Calculating the Period of Oscillation

The period of a physical pendulum can be determined using the formula:

T = 2π√(I / (mgh))

Where:

  • T = period of oscillation
  • I = moment of inertia about the pivot point
  • m = mass of the pendulum
  • g = acceleration due to gravity (approximately 9.81 m/s²)
  • h = distance from the pivot to the center of mass

Step 1: Finding the Mass of the Pendulum

First, we need to calculate the mass of the pendulum. The pipe has an inner radius of 10.2 cm and a thickness of 6.40 mm. The outer radius can be calculated as:

Outer radius = Inner radius + Thickness = 10.2 cm + 0.64 cm = 10.84 cm

Next, we can find the volume of the pipe section using the formula for the volume of a cylinder:

V = πh(R² - r²)

Where:

  • h = height of the pipe section (length)
  • R = outer radius
  • r = inner radius

Assuming the height of the pipe section is uniform and known, we can substitute the values to find the volume. Once we have the volume, we can multiply it by the density of the material (let's say the density of steel is approximately 7850 kg/m³) to find the mass.

Step 2: Calculating the Moment of Inertia

The moment of inertia for a cylindrical shell about its central axis is given by:

I = (1/2)m(R² + r²)

We will use the mass we calculated earlier and substitute the outer and inner radii to find the moment of inertia.

Step 3: Finding the Center of Mass

The center of mass for a uniform cylindrical shell is located at its midpoint. If the height of the pendulum is known, we can find the distance h from the pivot to the center of mass.

Step 4: Putting It All Together

Now that we have I, m, g, and h, we can substitute these values back into the period formula to find T.

Modifying the Pendulum

Now, let’s consider the modification where the bottom section of the pendulum is rotated 90° about a vertical axis through its center. This change will affect the moment of inertia and potentially the center of mass.

Analyzing the New Configuration

When the bottom section is rotated, the distribution of mass changes, which affects the moment of inertia. The new moment of inertia can be calculated similarly, but we need to account for the new orientation of the mass distribution.

To show that the new period of oscillation is about 2% less, we can calculate the new moment of inertia and center of mass, and then substitute these into the period formula again. The relationship between the two periods can be expressed as:

T_new = T_original * (1 - 0.02)

By performing the calculations, we can confirm that the new period is indeed approximately 2% less than the original period.

Conclusion

In summary, by carefully calculating the mass, moment of inertia, and center of mass for both the original and modified pendulum configurations, we can derive the periods of oscillation and understand how structural changes affect the dynamics of the system. This approach not only reinforces the principles of rotational motion but also illustrates the practical applications of physics in real-world scenarios.

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