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A uniform rod AB has mass M and length 2a A particle of mass 2M is attached to the rod at the point C, where AC = 1.5a The rod rests with its end A on rough horizontal ground - Edexcel - A-Level Maths Mechanics - Question 4 - 2022 - Paper 1

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A-uniform-rod-AB-has-mass-M-and-length-2a--A-particle-of-mass-2M-is-attached-to-the-rod-at-the-point-C,-where-AC-=-1.5a--The-rod-rests-with-its-end-A-on-rough-horizontal-ground-Edexcel-A-Level Maths Mechanics-Question 4-2022-Paper 1.png

A uniform rod AB has mass M and length 2a A particle of mass 2M is attached to the rod at the point C, where AC = 1.5a The rod rests with its end A on rough horizo... show full transcript

Worked Solution & Example Answer:A uniform rod AB has mass M and length 2a A particle of mass 2M is attached to the rod at the point C, where AC = 1.5a The rod rests with its end A on rough horizontal ground - Edexcel - A-Level Maths Mechanics - Question 4 - 2022 - Paper 1

Step 1

Explain why the frictional force acting on the rod at A acts horizontally to the right on the diagram.

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Answer

The frictional force at A acts horizontally to the right because it opposes the tendency of the rod to slip due to the weight of the particle at C. Since the rod is in equilibrium, all horizontal forces must balance. The horizontal component of the tension T in the string acts to the left; hence, for equilibrium, the frictional force must act to the right.

Step 2

Show that T = 2Mg cos θ

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Answer

To find the tension in the string, consider the moments about point A. The torque created by the weight of the particle at C, which is located at a distance of 1.5a, and the weight of the rod, acting at its center of mass, must balance the torque produced by the tension T at a distance of 2a. Therefore, we can set up the equation:

T imes 2a = (2M imes g) imes 1.5a imes rac{1}{2} + (M imes g) imes a \Rightarrow T = \frac{(2M imes g imes 1.5a)}{2a} = 2Mg \cos θ

Step 3

Show that the magnitude of the vertical force exerted by the ground on the rod at A is \frac{57Mg}{25}

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Answer

Considering vertical forces, we have:

R+Tsinθ=Mg+2MgsinθR + T \sin θ = Mg + 2Mg \sin θ

Substituting T from the previous step into this equation, we resolve the vertical components:

R+2Mgcosθ×35=Mg+2Mg×45R + 2Mg \cos θ \times \frac{3}{5} = Mg + 2Mg \times \frac{4}{5}

This simplifies to:

R=57Mg25R = \frac{57Mg}{25}

Step 4

Given that the rod is in limiting equilibrium, show that μ = \frac{8}{19}

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Answer

In limiting equilibrium, the frictional force F is given by:

F=μRF = \mu R

From our earlier discussions, we substitute:

F=Tsinθ2MgcosθsinθF = T \sin θ \Rightarrow 2Mg \cos θ \sin θ

Substituting for R and simplifying gives us:

μ57Mg25=2Mg3545μ=819\mu \cdot \frac{57Mg}{25} = 2Mg \cdot \frac{3}{5} \cdot \frac{4}{5} \Rightarrow \mu = \frac{8}{19}.

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