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A rough plane is inclined to the horizontal at an angle $\alpha$, where $\tan \alpha = \frac{3}{4}$ - Edexcel - A-Level Maths Mechanics - Question 2 - 2022 - Paper 1

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A rough plane is inclined to the horizontal at an angle $\alpha$, where $\tan \alpha = \frac{3}{4}$. A small block B of mass $5\,kg$ is held in equilibrium on the p... show full transcript

Worked Solution & Example Answer:A rough plane is inclined to the horizontal at an angle $\alpha$, where $\tan \alpha = \frac{3}{4}$ - Edexcel - A-Level Maths Mechanics - Question 2 - 2022 - Paper 1

Step 1

Find the magnitude of the frictional force acting on B

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Answer

To find the magnitude of the frictional force, we first need to resolve the forces acting on the block B along the inclined plane. The forces include the weight component down the slope and the applied horizontal force X.

Using geometry, we can determine that the weight W=mgW = mg can be resolved into two components:

  1. Down the slope: Wsin(α)=5gsin(α)W\sin(\alpha) = 5g\sin(\alpha)

  2. Perpendicular to the slope: Wcos(α)=5gcos(α)W\cos(\alpha) = 5g\cos(\alpha)

Substituting the normal reaction: N=68.6NN = 68.6\,N.

Using an(α)=34 an(\alpha) = \frac{3}{4}, we can derive rac{\sin(\alpha)}{\cos(\alpha)} = \frac{3}{4}. Therefore, sin(α)\sin(\alpha) and cos(α)\cos(\alpha) can be found using the triangle identity:

sin(α)=35 and cos(α)=45\sin(\alpha) = \frac{3}{5} \text{ and } \cos(\alpha) = \frac{4}{5}

Thus, the equation of motion perpendicular to the plane gives: 68.6=5gcos(α)68.6 = 5g\cos(\alpha) We can use the above equation to find g=9.8 m/s2g=9.8 \text{ m/s}^2.

The frictional force ff can then be expressed as: f = \mu N = 0.5 \cdot 68.6 = 34.3 N.

Step 2

State the direction of the frictional force acting on B

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Answer

The direction of the frictional force acting on block B will oppose the motion, which is down the incline. Thus, the frictional force acts up the plane.

Step 3

Find the acceleration of B down the plane

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Answer

Once the horizontal force X has been removed, the only forces acting on B will be its weight component down the slope, the frictional force, and the normal force.

The effective force down the slope can be expressed as:

Fnet=Wsin(α)fF_{net} = W\sin(\alpha) - f

Substituting the values we found: Fnet=(5gsin(α))34.3=(59.835)34.3F_{net} = (5g\sin(\alpha)) - 34.3 = (5 \cdot 9.8 \cdot \frac{3}{5}) - 34.3

Calculating gives: Fnet=29.434.3=4.9 NF_{net} = 29.4 - 34.3 = -4.9 \text{ N} This means that B is still moving down but with a net force of 4.9 N against the direction. Hence, this negative sign indicates the friction is greater than the component of the weight trying to pull B down the plane.

To find the acceleration, we can use Newton's second law:

F=maF = ma So, a=Fnetm=4.95=0.98 m/s2a = \frac{F_{net}}{m} = \frac{-4.9}{5} = -0.98 \text{ m/s}^2

The acceleration of B down the plane is thus 0.98 m/s2\approx -0.98 \text{ m/s}^2, indicating deceleration.

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