A L-shaped structure, OPQ can be rotated about O. OP and PQ measures 5 m and 1 m respectively. OP makes an acute angle, θ\theta, with the ground. The shortest distance from Q to the wall is LL m.

  1. (a)

    Show that L=5cos⁡θ−sin⁡θL = 5\cos\theta - \sin\theta.

  2. (b)

    Express LL in the form Rcos⁡(θ+α)R\cos(\theta+\alpha), where R>0R>0 and 0∘<α<90∘0^\circ<\alpha<90^\circ.

  3. (c)

    State the minimum value of LL and the corresponding value of θ\theta.

  4. (d)

    Find the value of θ\theta when L=3L = 3.

  5. (e)

    Explain why the maximum value of LL is not RR.

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Worked solution

10(a)

1. Find the horizontal distance from O to P.

Let the horizontal distance from O to P be x1x_1.
In the right-angled triangle formed by OP and the ground,
cos⁡θ=x15  ⟹  x1=5cos⁡θ\cos\theta = \frac{x_1}{5} \implies x_1 = 5\cos\theta

2. Find the horizontal distance from Q to P and subtract it to find L.

Let the horizontal distance from Q to P be x2x_2.
Since PQ is perpendicular to OP, the angle PQ makes with the vertical is θ\theta.
In the right-angled triangle formed by PQ and its horizontal/vertical components,
sin⁡θ=x21  ⟹  x2=sin⁡θ\sin\theta = \frac{x_2}{1} \implies x_2 = \sin\theta
Since Q is to the left of P, the horizontal distance from O to Q (which is the distance LL to the wall at O) is:
L=x1−x2=5cos⁡θ−sin⁡θL = x_1 - x_2 = 5\cos\theta - \sin\theta (Shown)

Answer

Shown

10(b)

1. Expand the target form and compare coefficients with the given expression

Rcos⁡(θ+α)=Rcos⁡θcos⁡α−Rsin⁡θsin⁡αR\cos(\theta+\alpha) = R\cos\theta\cos\alpha - R\sin\theta\sin\alpha
Comparing with L=5cos⁡θ−sin⁡θL = 5\cos\theta - \sin\theta:
Rcos⁡α=5R\cos\alpha = 5
Rsin⁡α=1R\sin\alpha = 1

2. Calculate the value of R

R=52+12=26≈5.0990R = \sqrt{5^2 + 1^2} = \sqrt{26} \approx 5.0990

3. Calculate the value of $\alpha$ and write the final expression

tan⁡α=15\tan\alpha = \frac{1}{5}
α=tan⁡−1(0.2)≈11.3099∘≈11.3∘\alpha = \tan^{-1}(0.2) \approx 11.3099^\circ \approx 11.3^\circ (to 1 d.p.)
L=26cos⁡(θ+11.3∘)L = \sqrt{26}\cos(\theta + 11.3^\circ)

Answer

26cos⁡(θ+11.3∘)\sqrt{26}\cos(\theta + 11.3^\circ)

10(c)

1. Identify the minimum value of the trigonometric expression

From part (b), L=26cos⁡(θ+11.31∘)L = \sqrt{26}\cos(\theta + 11.31^\circ).
The minimum value of a cosine function is −1-1.
Minimum value of L=−26L = -\sqrt{26}

2. Find the corresponding value of theta

For the minimum value, cos⁡(θ+11.31∘)=−1\cos(\theta + 11.31^\circ) = -1
θ+11.31∘=180∘\theta + 11.31^\circ = 180^\circ
θ=180∘−11.31∘=168.69∘≈168.7∘\theta = 180^\circ - 11.31^\circ = 168.69^\circ \approx 168.7^\circ

Answer

Minimum value of L=−26L = -\sqrt{26} (or −5.10-5.10), corresponding θ=168.7∘\theta = 168.7^\circ

10(d)

1. Set up the equation using the $R$-formula result from part (b)

From part (b), L=26cos⁡(θ+11.31∘)L = \sqrt{26}\cos(\theta + 11.31^\circ).
Given L=3L = 3, we have:
26cos⁡(θ+11.3099∘)=3\sqrt{26}\cos(\theta + 11.3099^\circ) = 3
cos⁡(θ+11.3099∘)=326\cos(\theta + 11.3099^\circ) = \frac{3}{\sqrt{26}}

2. Solve for the acute angle $\theta$

θ+11.3099∘=cos⁡−1(326)\theta + 11.3099^\circ = \cos^{-1}\left(\frac{3}{\sqrt{26}}\right)
θ+11.3099∘≈53.960∘\theta + 11.3099^\circ \approx 53.960^\circ
θ=53.960∘−11.3099∘=42.650∘≈42.7∘\theta = 53.960^\circ - 11.3099^\circ = 42.650^\circ \approx 42.7^\circ

Answer

42.7∘42.7^\circ

10(e)

1. Identify the condition for $L$ to reach its theoretical maximum of $R$

For L=Rcos⁡(θ+α)L = R\cos(\theta + \alpha) to reach its maximum value of RR, we must have cos⁡(θ+α)=1\cos(\theta + \alpha) = 1.
This occurs when θ+α=0∘\theta + \alpha = 0^\circ, which means θ=−α\theta = -\alpha.

2. Explain why this condition is impossible given the context

The question states that θ\theta is an acute angle, so 0∘<θ<90∘0^\circ < \theta < 90^\circ.
Since α>0∘\alpha > 0^\circ, θ\theta would have to be negative to satisfy θ=−α\theta = -\alpha.
Therefore, θ\theta cannot take the value required to make L=RL = R.

Answer

For LL to be maximum (L=RL = R), cos⁡(θ+α)\cos(\theta + \alpha) must be 11, which requires θ+α=0∘  ⟹  θ=−α\theta + \alpha = 0^\circ \implies \theta = -\alpha. Since θ\theta is an acute angle (0∘<θ<90∘0^\circ < \theta < 90^\circ), it cannot be negative, so LL cannot reach RR.

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