The diagram shows an area that is enclosed by glass panels at ABAB, BCBC and ADAD. AB=10 mAB = 10\text{ m}, AD=30 mAD = 30\text{ m}, angle DAB=angle BCD=90∘DAB = \text{angle } BCD = 90^\circ. The glass panel ADAD makes an acute angle θ\theta with CDCD.

  1. (i)

    Show that L mL\text{ m}, the length of the glass panels, can be expressed as 40+30sin⁡θ−10cos⁡θ40 + 30\sin\theta - 10\cos\theta.

  2. (ii)

    Express LL in the form 40+Rsin⁡(θ−α)40 + R\sin(\theta - \alpha) where R>0R > 0 and 0∘<α<90∘0^\circ < \alpha < 90^\circ.

  3. (iii)

    The total length of the glass panels is 65 m. Find the value of θ\theta.

  4. (iv)

    Explain whether it is possible to build an area where the length of the glass panels is 90 m.

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Worked solution

12(i)

1. Express the length of the glass panels in terms of the given sides.

The total length of the glass panels is L=AB+BC+ADL = AB + BC + AD.
Given AB=10AB = 10 and AD=30AD = 30,
L=10+BC+30=40+BCL = 10 + BC + 30 = 40 + BC.

2. Find the length of BC by projecting AD and AB onto the vertical axis.

Draw a horizontal line through AA and a vertical line through DD to form a right-angled triangle with ADAD. The vertical height of AA above CDCD is ADsin⁡θ=30sin⁡θAD \sin\theta = 30\sin\theta.
Since ∠DAB=90∘\angle DAB = 90^\circ, the angle ABAB makes with the vertical is θ\theta.
The vertical drop from AA to BB is ABcos⁡θ=10cos⁡θAB \cos\theta = 10\cos\theta.
Therefore, the vertical height of BB above CDCD (which is the length of BCBC) is:
BC=30sin⁡θ−10cos⁡θBC = 30\sin\theta - 10\cos\theta.

3. Substitute BC into the expression for L to complete the proof.

L=40+(30sin⁡θ−10cos⁡θ)L = 40 + (30\sin\theta - 10\cos\theta)
L=40+30sin⁡θ−10cos⁡θL = 40 + 30\sin\theta - 10\cos\theta (Shown)

Answer

L=40+30sin⁡θ−10cos⁡θL = 40 + 30\sin\theta - 10\cos\theta (Shown)

12(ii)

1. Set up the R-formula equation for the trigonometric part

Let 30sin⁡θ−10cos⁡θ=Rsin⁡(θ−α)30\sin\theta - 10\cos\theta = R\sin(\theta - \alpha).
Expanding the right side gives:
30sin⁡θ−10cos⁡θ=R(sin⁡θcos⁡α−cos⁡θsin⁡α)30\sin\theta - 10\cos\theta = R(\sin\theta\cos\alpha - \cos\theta\sin\alpha)
Comparing coefficients:
Rcos⁡α=30R\cos\alpha = 30
Rsin⁡α=10R\sin\alpha = 10

2. Calculate the value of R

R=302+102R = \sqrt{30^2 + 10^2}
R=900+100=1000=1010≈31.623R = \sqrt{900 + 100} = \sqrt{1000} = 10\sqrt{10} \approx 31.623

3. Calculate the value of alpha

tan⁡α=1030=13\tan\alpha = \frac{10}{30} = \frac{1}{3}
Since 0∘<α<90∘0^\circ < \alpha < 90^\circ,
α=tan⁡−1(13)≈18.435∘\alpha = \tan^{-1}\left(\frac{1}{3}\right) \approx 18.435^\circ

4. State the final expression for L

L=40+31.6sin⁡(θ−18.4∘)L = 40 + 31.6\sin(\theta - 18.4^\circ) (to 3 s.f. and 1 d.p. respectively)

Answer

40+31.6sin⁡(θ−18.4∘)40 + 31.6\sin(\theta - 18.4^\circ)

12(iii)

1. Find the values of $R$ and $\alpha$ from part (ii)

From part (ii), 30sin⁡θ−10cos⁡θ=Rsin⁡(θ−α)30\sin\theta - 10\cos\theta = R\sin(\theta - \alpha).
R=302+102=1000=1010R = \sqrt{30^2 + 10^2} = \sqrt{1000} = 10\sqrt{10}
tan⁡α=1030=13  ⟹  α≈18.435∘\tan\alpha = \frac{10}{30} = \frac{1}{3} \implies \alpha \approx 18.435^\circ
So, L=40+1000sin⁡(θ−18.435∘)L = 40 + \sqrt{1000}\sin(\theta - 18.435^\circ)

2. Set up the equation for $L = 65$ and isolate the sine term

40+1000sin⁡(θ−18.435∘)=6540 + \sqrt{1000}\sin(\theta - 18.435^\circ) = 65
1000sin⁡(θ−18.435∘)=25\sqrt{1000}\sin(\theta - 18.435^\circ) = 25
sin⁡(θ−18.435∘)=251000\sin(\theta - 18.435^\circ) = \frac{25}{\sqrt{1000}}

3. Solve for $\theta$

θ−18.435∘=sin⁡−1(251000)\theta - 18.435^\circ = \sin^{-1}\left(\frac{25}{\sqrt{1000}}\right)
θ−18.435∘≈52.239∘\theta - 18.435^\circ \approx 52.239^\circ
θ≈70.674∘≈70.7∘\theta \approx 70.674^\circ \approx 70.7^\circ (to 1 d.p.)
(The other solution θ−18.435∘=180∘−52.239∘=127.761∘  ⟹  θ=146.2∘\theta - 18.435^\circ = 180^\circ - 52.239^\circ = 127.761^\circ \implies \theta = 146.2^\circ is rejected as θ\theta is acute)

Answer

70.7∘70.7^\circ

12(iv)

1. Determine the maximum value of the expression for L

From (ii), L=40+1000sin⁡(θ−18.43∘)=40+1010sin⁡(θ−18.43∘)L = 40 + \sqrt{1000}\sin(\theta - 18.43^\circ) = 40 + 10\sqrt{10}\sin(\theta - 18.43^\circ).
The maximum value of sin⁡(θ−18.43∘)\sin(\theta - 18.43^\circ) is 1.
Maximum L=40+1010≈71.62 mL = 40 + 10\sqrt{10} \approx 71.62\text{ m}.

2. Compare the maximum length with 90 m and conclude

Since 71.62 m<90 m71.62\text{ m} < 90\text{ m}, it is not possible for the length of the glass panels to be 90 m.

Answer

No, because the maximum possible length of the glass panels is 40+1010≈71.6 m40 + 10\sqrt{10} \approx 71.6\text{ m}, which is less than 90 m90\text{ m}.

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