图中显示了一个靠在垂直墙上的长方形 ABCDABCD。 ABAB 为 10 米,ADAD 为 3 米,且边 BCBC 与地面成 θ∘\theta^\circ 的角。
ECEC 为 CC 到墙的水平距离。
只要 ECEC 介于 7.5 米和 9.5 米之间,长方形 ABCDABCD 就会保持靠在墙上。

  1. (i)

    证明 ECEC 可以表示为 asin⁡θ+bcos⁡θa \sin \theta + b \cos \theta 的形式,其中 aa 和 bb 为待求常数。

  2. (ii)

    将 ECEC 表示为 Rsin⁡(θ+α)R \sin (\theta + \alpha) 的形式,其中 R>0R > 0 且 α\alpha 为锐角。

  3. (iii)

    求长方形 ABCDABCD 保持靠在墙上的 θ\theta 的取值范围。

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完整解法

11(i)

1. Find the horizontal distance from the wall to point B.

Let the corner where the wall meets the floor be OO. In the right-angled triangle AOBAOB, the angle OBAOBA and the angle θ\theta that BCBC makes with the floor are complementary because ∠ABC=90∘\angle ABC = 90^\circ and the floor is a straight line.
Therefore, ∠OBA=180∘−90∘−θ=90∘−θ\angle OBA = 180^\circ - 90^\circ - \theta = 90^\circ - \theta.
The horizontal distance OBOB is given by:
OB=ABcos⁡(90∘−θ)=10sin⁡θOB = AB \cos(90^\circ - \theta) = 10 \sin \theta

2. Find the horizontal distance from B to C and sum them to find EC.

The horizontal distance from BB to CC is the projection of BCBC onto the horizontal floor.
Since ABCDABCD is a rectangle, BC=AD=3BC = AD = 3 m.
Horizontal projection of BC=BCcos⁡θ=3cos⁡θBC = BC \cos \theta = 3 \cos \theta.
The total horizontal distance ECEC from the wall to CC is the sum of the horizontal distance to BB and the horizontal projection of BCBC:
EC=OB+3cos⁡θ=10sin⁡θ+3cos⁡θEC = OB + 3 \cos \theta = 10 \sin \theta + 3 \cos \theta
Comparing with asin⁡θ+bcos⁡θa \sin \theta + b \cos \theta, we have a=10a = 10 and b=3b = 3.

答案

EC=10sin⁡θ+3cos⁡θEC = 10 \sin \theta + 3 \cos \theta
a=10a = 10, b=3b = 3

11(ii)

1. Identify the expression for $EC$ from part (i) and set up the R-formula equation

From part (i), EC=10sin⁡θ+3cos⁡θEC = 10 \sin \theta + 3 \cos \theta.
Let 10sin⁡θ+3cos⁡θ=Rsin⁡(θ+α)=Rsin⁡θcos⁡α+Rcos⁡θsin⁡α10 \sin \theta + 3 \cos \theta = R \sin (\theta + \alpha) = R \sin \theta \cos \alpha + R \cos \theta \sin \alpha.

2. Find the value of $R$

Comparing coefficients:
Rcos⁡α=10R \cos \alpha = 10
Rsin⁡α=3R \sin \alpha = 3
R=102+32=109R = \sqrt{10^2 + 3^2} = \sqrt{109}

3. Find the value of $\alpha$

tan⁡α=310=0.3\tan \alpha = \frac{3}{10} = 0.3
α=tan⁡−1(0.3)≈16.699∘≈16.7∘\alpha = \tan^{-1}(0.3) \approx 16.699^\circ \approx 16.7^\circ (to 1 d.p.)

4. State the final expression

EC=109sin⁡(θ+16.7∘)EC = \sqrt{109} \sin (\theta + 16.7^\circ)

答案

EC=109sin⁡(θ+16.7∘)EC = \sqrt{109} \sin (\theta + 16.7^\circ)

11(iii)

1. Set up the inequality using the condition given and the result from part (ii).

From part (ii), EC=109sin⁡(θ+16.7∘)EC = \sqrt{109} \sin (\theta + 16.7^\circ).
Given 7.5⩽EC⩽9.57.5 \leqslant EC \leqslant 9.5,
7.5⩽109sin⁡(θ+16.699∘)⩽9.57.5 \leqslant \sqrt{109} \sin (\theta + 16.699^\circ) \leqslant 9.5

2. Solve for the lower bound of $\theta$.

109sin⁡(θ+16.699∘)⩾7.5\sqrt{109} \sin (\theta + 16.699^\circ) \geqslant 7.5
sin⁡(θ+16.699∘)⩾7.5109\sin (\theta + 16.699^\circ) \geqslant \frac{7.5}{\sqrt{109}}
θ+16.699∘⩾sin⁡−1(7.5109)\theta + 16.699^\circ \geqslant \sin^{-1}\left(\frac{7.5}{\sqrt{109}}\right)
θ+16.699∘⩾45.919∘\theta + 16.699^\circ \geqslant 45.919^\circ
θ⩾29.220∘\theta \geqslant 29.220^\circ

3. Solve for the upper bound of $\theta$.

109sin⁡(θ+16.699∘)⩽9.5\sqrt{109} \sin (\theta + 16.699^\circ) \leqslant 9.5
sin⁡(θ+16.699∘)⩽9.5109\sin (\theta + 16.699^\circ) \leqslant \frac{9.5}{\sqrt{109}}
θ+16.699∘⩽sin⁡−1(9.5109)\theta + 16.699^\circ \leqslant \sin^{-1}\left(\frac{9.5}{\sqrt{109}}\right)
θ+16.699∘⩽65.496∘\theta + 16.699^\circ \leqslant 65.496^\circ
θ⩽48.797∘\theta \leqslant 48.797^\circ

4. State the final range of values for $\theta$.

29.2∘⩽θ⩽48.8∘ (to 1 d.p.)29.2^\circ \leqslant \theta \leqslant 48.8^\circ \text{ (to 1 d.p.)}

答案

29.2∘⩽θ⩽48.8∘29.2^\circ \leqslant \theta \leqslant 48.8^\circ

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