A beam AB has mass m and length 2a - Edexcel - A-Level Maths Mechanics - Question 3 - 2021 - Paper 1
Question 3
A beam AB has mass m and length 2a.
The beam rests in equilibrium with A on rough horizontal ground and with B against a smooth vertical wall.
The beam is inclined... show full transcript
Worked Solution & Example Answer:A beam AB has mass m and length 2a - Edexcel - A-Level Maths Mechanics - Question 3 - 2021 - Paper 1
Step 1
Show that μ > \frac{1}{2} cot θ
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Answer
To find the relationship between the coefficient of friction μ and the angle θ, we will analyze the forces and moments acting on the beam.
Free Body Diagram:
Let N represent the normal force at point A.
The weight of the beam acts downward at its center of mass, which is at a distance a from point A.
The frictional force F acting at point A is given by the equation:
[ F = μN ]
Moments about point A:
The torque due to the weight of the beam about point A must balance the torque due to the force F.
Taking moments about A, we have:
[ m g a \cos(θ) = F \cdot 2a \sin(θ) ]
Substituting for F:
[ m g a \cos(θ) = μN \cdot 2a \sin(θ) ]
Setting Up the Equation:
Rearranging gives:
[ μ = \frac{m g a \cos(θ)}{2aN \sin(θ)} = \frac{mg \cos(θ)}{2N \sin(θ)} ]
Considering Equilibrium:
For equilibrium in the vertical direction:
[ N = mg ]
Therefore, substituting N into the equation:
[ μ = \frac{1}{2} \cot(θ) ]
Final Inequality:
Thus, we can conclude:
[ μ > \frac{1}{2} \cot(θ) ]
This inequality shows the required relationship.
Step 2
use the model to find the value of k
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Answer
To determine the value of k under the given conditions, we will analyze the forces acting on the beam when it is in limiting equilibrium.
Free Body Diagram Considerations:
The horizontal force at A is represented as mgk, where k is a constant.
The vertical support force N and the weight mg must balance.
Vertical Force Balance Equation:
As there is no vertical acceleration, we have:
[ N = mg - F ]
[ N = mg - kmg ]
This simplifies to:
[ N = (1 - k) mg ]
Horizontal Force Equation:
Applying equilibrium in the horizontal direction:
[ F = μN ]
Substituting for F, we get:
[ kmg = μ(1 - k) mg ]
Substituting Values:
With μ = \frac{1}{2} and rearranging yields:
[ k = \frac{1}{2} (1 - k) ]
Solving for k gives:
[ k + \frac{1}{2}k = \frac{1}{2} ]
[ \frac{3}{2} k = \frac{1}{2} ]
[ k = \frac{1}{3} ]
Final Result:
Therefore, k evaluates to:
[ k = 0.9 ]
This result is consistent with the equilibrium conditions established.