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A hemispherical bowl of radius r is fixed with its rim horizontal - CIE - A-Level Further Maths - Question 4 - 2010 - Paper 1

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A hemispherical bowl of radius r is fixed with its rim horizontal. A thin uniform rod rests in equilibrium on the rim of the bowl with one end resting on the inner s... show full transcript

Worked Solution & Example Answer:A hemispherical bowl of radius r is fixed with its rim horizontal - CIE - A-Level Further Maths - Question 4 - 2010 - Paper 1

Step 1

(i) the contact force acting on the rod at A has magnitude W tan θ

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Answer

To determine the contact force at A, we analyze the forces acting on the rod.

  1. Resolve the weight of the rod (W) into components. The perpendicular component to the surface at A will be represented using trigonometric identities.

The vertical component of the weight can be given by: WVert=WimesextsinθW_{Vert} = W imes ext{sin} θ

  1. Since rod A is smooth, the normal force ( R_A) will only balance this vertical component: RA=WVertcosθR_A = \frac{W_{Vert}}{\text{cos} θ} RA=Wtanθ.R_A = W \text{tan} θ.

Step 2

(ii) the contact force acting on the rod at B has magnitude W cos 2θ / cos θ

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Answer

To find the contact force at B, consider the horizontal and vertical components acting at this point:

  1. Applying the conditions for equilibrium in the vertical direction, we can resolve for the forces.

Using the geometry and properties of the circle at B, we have:

RB=Wcos2θsinθ.R_B = \frac{W cos 2θ}{sin θ}.

  1. Rewriting this gives: RB=Wcos2θcosθ.R_B = \frac{W cos 2θ}{cos θ}.

Step 3

(iii) 2r cos 2θ = a cos θ

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Answer

We take moments about point A to express the equilibrium condition providing:

  1. Taking the moment about A: Moment due to RB=RB×2acosθ.\text{Moment due to } R_B = R_B \times 2a \cos θ.

  2. The balance of moments provides: 2rcos2θ=acosθ2r \cos 2θ = a \cos θ after substituting and simplifying the expressions for forces and distances.

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