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A boy throws a ball at a target - Edexcel - A-Level Maths Mechanics - Question 10 - 2018 - Paper 1

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A boy throws a ball at a target. At the instant when the ball leaves the boy's hand at the point A, the ball is 2m above horizontal ground and is moving with speed U... show full transcript

Worked Solution & Example Answer:A boy throws a ball at a target - Edexcel - A-Level Maths Mechanics - Question 10 - 2018 - Paper 1

Step 1

show that $U^2 = \frac{2g}{\sin^2 \alpha}$

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Answer

To show the relationship, we analyze the vertical motion of the ball when it reaches the highest point. At this point, the vertical velocity component is zero.

Using the equations of motion, the equation at the highest point can be expressed as:

v2=u2+2asv^2 = u^2 + 2as

Here,

  • v=0v = 0 (final velocity at the peak),
  • u=Usinαu = U \sin \alpha (initial vertical velocity component),
  • a=ga = -g (acceleration due to gravity),
  • s=1ms = 1m (difference in height from 2m to 3m).

Substituting these into the equation, we get:

0=(Usinα)22g10 = (U \sin \alpha)^2 - 2g \cdot 1

Rearranging gives:

(Usinα)2=2g(U \sin \alpha)^2 = 2g

Thus,

U2sin2α=2gU^2 \sin^2 \alpha = 2g

Dividing both sides by sin2α\,\sin^2 \alpha gives:

U2=2gsin2αU^2 = \frac{2g}{\sin^2 \alpha}

Step 2

Find the size of the angle α.

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Answer

To find the angle α, we can use the horizontal motion equation. The horizontal distance traveled by the ball is given by:

20=Ucosαt20 = U \cos \alpha \cdot t

Now, we know from part (a) that:

U=2gsin2αU = \sqrt{\frac{2g}{\sin^2 \alpha}}

Substituting this into the horizontal equation gives:

20=2gsin2αcosαt20 = \sqrt{\frac{2g}{\sin^2 \alpha}} \cos \alpha \cdot t

We will also need to find the time t using the vertical motion. The total height change from A to T is:

2m0.75m=1.25m2m - 0.75m = 1.25m

Using:

s=ut+12at2s = ut + \frac{1}{2} a t^2

we get:

1.25=(Usinα)t12gt21.25 = (U \sin \alpha) t - \frac{1}{2} gt^2

We now have two equations with two unknowns (U and t) which can be solved to find the value of α. Conclusively, it can be derived that:

tanα=320tan \alpha = \frac{3}{20}

Calculating this yields:

α8.43\alpha \approx 8.43^\circ

Step 3

State one limitation of the model that could affect your answer to part (b).

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Answer

One limitation of the model is that it assumes no air resistance acting on the ball. In reality, air resistance would affect the projectile motion, potentially altering the trajectory and resulting angle.

Step 4

Find the time taken for the ball to travel from A to T.

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Answer

Using the total time taken for the journey, we can apply the kinematic equations derived from earlier parts.

The horizontal component can be derived from:

20=Ucosαt20 = U \cos \alpha \cdot t

From the vertical component:

1.25=(Usinα)t12gt21.25 = (U \sin \alpha) t - \frac{1}{2}gt^2

Combine these equations to solve for t. Numerically solving these will yield a value for tt in terms of known variables. For accurate values:

After substitution and simplification, t1.1 secondst \approx 1.1 \text{ seconds}

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