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8. (a) Prove that the moment of inertia of a uniform rod, of mass m and length 2l about an axis through its centre, perpendicular to the rod, is \( \frac{1}{3}ml^2 \) - Leaving Cert Applied Maths - Question 8 - 2019

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8.-(a)-Prove-that-the-moment-of-inertia-of-a-uniform-rod,-of-mass-m-and-length-2l-about-an-axis-through-its-centre,-perpendicular-to-the-rod,-is-\(-\frac{1}{3}ml^2-\)-Leaving Cert Applied Maths-Question 8-2019.png

8. (a) Prove that the moment of inertia of a uniform rod, of mass m and length 2l about an axis through its centre, perpendicular to the rod, is \( \frac{1}{3}ml^2 \... show full transcript

Worked Solution & Example Answer:8. (a) Prove that the moment of inertia of a uniform rod, of mass m and length 2l about an axis through its centre, perpendicular to the rod, is \( \frac{1}{3}ml^2 \) - Leaving Cert Applied Maths - Question 8 - 2019

Step 1

Prove that the moment of inertia of a uniform rod, of mass m and length 2l about an axis through its centre, perpendicular to the rod

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Answer

To prove that the moment of inertia ( I ) of a uniform rod about an axis through its center, perpendicular to the rod, we can start by defining the mass per unit length as:

[ M = \frac{m}{2l} ]

Next, we consider a differential element of the rod:

  • Let ( dx ) be a small segment around the center.
  • The moment of inertia of this element about the center is given by:

[ dI = M \cdot dx \cdot x^2 ]

Thus, the total moment of inertia of the rod can be determined by integrating over its length:

[ I = \int_{-l}^{l} dI = M \int_{-l}^{l} x^2 dx ]

Calculating the integral yields:

[ I = \frac{M}{3} [x^3]_{-l}^{l} = \frac{M}{3} (l^3 - (-l)^3) = \frac{2Ml^3}{3} ]

Inserting ( M = \frac{m}{2l} ) gives:

[ I = \frac{1}{3} ml^2 ]

Step 2

Find (i) the moment of inertia of the compound body about the axis of rotation

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Answer

To determine the moment of inertia ( I_a ) of the compound body about the axis of rotation located at point A, we consider the contributions from both the rod and the disc:

  • The moment of inertia of the rod about its own center is:

[ I_{rod} = \frac{1}{3} m(0.5)^2 + m(0.5)(1.1^2) ]

Calculating:

[ = \frac{1}{3} m(0.25) + m(0.5)(1.21) ] [ = \frac{m}{12} + 1.21m = 1.548m ]

Thus, the total moment of inertia is:

[ I_a = 1.548m ]

Step 3

Find (ii) the period of small oscillations correct to two decimal places

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Answer

Given that the oscillation occurs about a horizontal axis:

Using the formula for the period of a physical pendulum, where ( mgh = mgx ):

[ Mg h = mg(0.5) + mg(1.1) ] [ = 1.6mg ]

Thus, the period ( T ) is given by:

[ T = 2\pi \sqrt{\frac{I}{mg}} ]

Substituting the values gives:

[ T = 2\pi \sqrt{\frac{929m}{600\times 1.6g}} ] [ = 1.97s ]

Step 4

Find (iii) the length of the equivalent simple pendulum

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Answer

To find the length ( L ) of the equivalent simple pendulum, we relate it as follows:

[ 2\pi \sqrt{\frac{L}{g}} = T ]

Thus,

[ L = \left(\frac{T}{2\pi}\right)^2 g ]

Calculating gives:

[ L = \left(\frac{1.97}{2\pi}\right)^2 g ] [ = 0.97m ]

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