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In the diagram, D, B and C are points in the same horizontal plane. AB is a vertical flagpole. A rope is tied from A, the top of the flagpole, to point C. BAC = BCD = θ, BDC = α and AB = 4 units.

Mathematics

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Answer

sin⁡T^t=sin⁡P^p\frac{\sin \hat{T}}{t} = \frac{\sin \hat{P}}{p}

BC=4tan⁡θBC = 4 \tan \theta

DC=4sin⁡θ(1+tan⁡θtan⁡α)DC = 4 \sin \theta \left(1 + \frac{\tan \theta}{\tan \alpha}\right)

Step-by-step solution

9 steps

QUESTION 8

8.1 Prove that sin⁡T^t=sin⁡P^p\frac{\sin \hat{T}}{t} = \frac{\sin \hat{P}}{p}.

  1. Draw an altitude from R to the line TP.

    Let H be the foot of the perpendicular from R to TP. So, RH is the altitude.
    In right-angled △RHT\triangle RHT:

    sin⁡T^=RHRT\sin \hat{T} = \frac{RH}{RT}

    Given RT=pRT = p, so:

    sin⁡T^=RHp  ⟹  RH=psin⁡T^(Equation 1)\sin \hat{T} = \frac{RH}{p} \implies RH = p \sin \hat{T} \quad \text{(Equation 1)}
  2. Use the altitude in the other right-angled triangle.

    In right-angled △RHP\triangle RHP:

    sin⁡P^=RHRP\sin \hat{P} = \frac{RH}{RP}

    Given RP=tRP = t, so:

    sin⁡P^=RHt  ⟹  RH=tsin⁡P^(Equation 2)\sin \hat{P} = \frac{RH}{t} \implies RH = t \sin \hat{P} \quad \text{(Equation 2)}
  3. Equate the expressions for RH and rearrange.

    From Equation 1 and Equation 2:

    psin⁡T^=tsin⁡P^p \sin \hat{T} = t \sin \hat{P}

    Divide both sides by ptpt:

    psin⁡T^pt=tsin⁡P^pt\frac{p \sin \hat{T}}{pt} = \frac{t \sin \hat{P}}{pt} sin⁡T^t=sin⁡P^p\frac{\sin \hat{T}}{t} = \frac{\sin \hat{P}}{p}

    This proves the identity.

    sin⁡T^t=sin⁡P^p\boxed{\frac{\sin \hat{T}}{t} = \frac{\sin \hat{P}}{p}}

    8.2.1 Show that the distance between B and C is 4tan⁡θ4 \tan \theta.

  4. Identify the relevant triangle and its properties.

    Consider △ABC\triangle ABC. AB is a vertical flagpole and B, C are points in the horizontal plane, so ∠ABC=90∘\angle ABC = 90^\circ.
    We are given AB=4AB = 4 units and BA^C=θ\text{B}\hat{\text{A}}\text{C} = \theta.

  5. Use a trigonometric ratio to find BC.

    In right-angled △ABC\triangle ABC:

    tan⁡(BA^C)=OppositeAdjacent=BCAB\tan(\text{B}\hat{\text{A}}\text{C}) = \frac{\text{Opposite}}{\text{Adjacent}} = \frac{BC}{AB}

    Substitute the given values:

    tan⁡θ=BC4\tan \theta = \frac{BC}{4} BC=4tan⁡θBC = 4 \tan \theta

    This shows that the distance between B and C is 4tan⁡θ4 \tan \theta.

    BC=4tan⁡θ\boxed{BC = 4 \tan \theta}

    8.2.2 Hence, show that DC=4sin⁡θ(1+tan⁡θtan⁡α)\text{DC} = 4 \sin \theta \left(1 + \frac{\tan \theta}{\tan \alpha}\right).

  6. Use the Sine Rule in △BCD\triangle BCD.

    We have BC=4tan⁡θBC = 4 \tan \theta from 8.2.1.
    In △BCD\triangle BCD, we are given BC^D=θ\text{B}\hat{\text{C}}\text{D} = \theta and BD^C=α\text{B}\hat{\text{D}}\text{C} = \alpha.
    The sum of angles in a triangle is 180∘180^\circ, so DB^C=180∘−(θ+α)\text{D}\hat{\text{B}}\text{C} = 180^\circ - (\theta + \alpha).
    Using the Sine Rule:

    DCsin⁡(DB^C)=BCsin⁡(BD^C)\frac{DC}{\sin(\text{D}\hat{\text{B}}\text{C})} = \frac{BC}{\sin(\text{B}\hat{\text{D}}\text{C})} DCsin⁡(180∘−(θ+α))=BCsin⁡α\frac{DC}{\sin(180^\circ - (\theta + \alpha))} = \frac{BC}{\sin \alpha}

    Since sin⁡(180∘−X)=sin⁡X\sin(180^\circ - X) = \sin X:

    DCsin⁡(θ+α)=BCsin⁡α\frac{DC}{\sin(\theta + \alpha)} = \frac{BC}{\sin \alpha}
  7. Substitute BCBC and solve for DCDC.

    DC=BCsin⁡(θ+α)sin⁡αDC = \frac{BC \sin(\theta + \alpha)}{\sin \alpha}

    Substitute BC=4tan⁡θBC = 4 \tan \theta:

    DC=4tan⁡θsin⁡(θ+α)sin⁡αDC = \frac{4 \tan \theta \sin(\theta + \alpha)}{\sin \alpha}
  8. Expand sin⁡(θ+α)\sin(\theta + \alpha) and simplify.

    DC=4tan⁡θ(sin⁡θcos⁡α+cos⁡θsin⁡α)sin⁡αDC = \frac{4 \tan \theta (\sin \theta \cos \alpha + \cos \theta \sin \alpha)}{\sin \alpha} DC=4tan⁡θ(sin⁡θcos⁡αsin⁡α+cos⁡θsin⁡αsin⁡α)DC = 4 \tan \theta \left( \frac{\sin \theta \cos \alpha}{\sin \alpha} + \frac{\cos \theta \sin \alpha}{\sin \alpha} \right) DC=4tan⁡θ(sin⁡θcot⁡α+cos⁡θ)DC = 4 \tan \theta \left( \sin \theta \cot \alpha + \cos \theta \right)
  9. Manipulate the expression to match the required form.

    Recall tan⁡θ=sin⁡θcos⁡θ\tan \theta = \frac{\sin \theta}{\cos \theta} and cot⁡α=1tan⁡α\cot \alpha = \frac{1}{\tan \alpha}.

    DC=4sin⁡θcos⁡θ(sin⁡θ1tan⁡α+cos⁡θ)DC = 4 \frac{\sin \theta}{\cos \theta} \left( \sin \theta \frac{1}{\tan \alpha} + \cos \theta \right)

    Factor out cos⁡θ\cos \theta from the bracket:

    DC=4sin⁡θcos⁡θcos⁡θ(sin⁡θcos⁡θtan⁡α+1)DC = 4 \frac{\sin \theta}{\cos \theta} \cos \theta \left( \frac{\sin \theta}{\cos \theta \tan \alpha} + 1 \right) DC=4sin⁡θ(tan⁡θtan⁡α+1)DC = 4 \sin \theta \left( \frac{\tan \theta}{\tan \alpha} + 1 \right) DC=4sin⁡θ(1+tan⁡θtan⁡α)DC = 4 \sin \theta \left( 1 + \frac{\tan \theta}{\tan \alpha} \right)

    This shows the required expression for DC.

    DC=4sin⁡θ(1+tan⁡θtan⁡α)\boxed{DC = 4 \sin \theta \left(1 + \frac{\tan \theta}{\tan \alpha}\right)}
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