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Question Number 39985 by ajfour last updated on 14/Jul/18

Answered by ajfour last updated on 15/Jul/18

eq. of line  OBC :  y=x  eq. of AEC:    ytan θ=x−1  For point C :       x_C =y_C =(1/(1−tan θ))    ∠ADB =θ  so AD= cot θ  slope of CD be m         −m=(y_C /(1+cot θ−x_C ))                =(1/((1+cot θ)(1−tan θ)−1))             = (1/(−tan θ+cot θ−1))  tan ∠DAF = (1/m) =1+tan θ−cot θ  FD =ADsin ∠DAF          =cot θ×((1+tan θ−cot θ)/(√(1+(1+tan θ−cot θ)^2 )))  ∠BCE =(π/4)−θ      CE =BEcot ((π/4)−θ)               =((sin θ)/(tan ((π/4)−θ)))    Given CE = FD  ⇒ ((sin θ)/(tan ((π/4)−θ)))=cot θ×((1+tan θ−cot θ)/(√(1+(1+tan θ−cot θ)^2 )))  ⇒ ((sin θ(1+tan θ)tan θ)/(1−tan θ))=((1+tan θ−cot θ)/(√(1+(1+tan θ−cot θ)^2 )))  let  tan θ=t  ⇒  sin θ = (t/(√(1+t^2 )))  ⇒ ((t(1+t)t)/((√(1+t^2 ))(1−t)))=((1+t−(1/t))/(√(1+(1+t−(1/t))^2 )))  ⇒ ((t^4 (1+t)^2 )/((1+t^2 )(1−t)^2 ))=(((t+t^2 −1)^2 )/(t^2 +(t+t^2 −1)^2 ))  ⇒ t=tan θ ≈ 0.63923        θ ≈ 32.588° .

$${eq}.\:{of}\:{line}\:\:{OBC}\::\:\:{y}={x} \\ $$$${eq}.\:{of}\:{AEC}:\:\:\:\:{y}\mathrm{tan}\:\theta={x}−\mathrm{1} \\ $$$${For}\:{point}\:{C}\:: \\ $$$$\:\:\:\:\:{x}_{{C}} ={y}_{{C}} =\frac{\mathrm{1}}{\mathrm{1}−\mathrm{tan}\:\theta}\:\: \\ $$$$\angle{ADB}\:=\theta \\ $$$${so}\:{AD}=\:\mathrm{cot}\:\theta \\ $$$${slope}\:{of}\:{CD}\:{be}\:{m} \\ $$$$\:\:\:\:\:\:\:−{m}=\frac{{y}_{{C}} }{\mathrm{1}+\mathrm{cot}\:\theta−{x}_{{C}} } \\ $$$$\:\:\:\:\:\:\:\:\:\:\:\:\:\:=\frac{\mathrm{1}}{\left(\mathrm{1}+\mathrm{cot}\:\theta\right)\left(\mathrm{1}−\mathrm{tan}\:\theta\right)−\mathrm{1}} \\ $$$$\:\:\:\:\:\:\:\:\:\:\:=\:\frac{\mathrm{1}}{−\mathrm{tan}\:\theta+\mathrm{cot}\:\theta−\mathrm{1}} \\ $$$$\mathrm{tan}\:\angle{DAF}\:=\:\frac{\mathrm{1}}{{m}}\:=\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta \\ $$$${FD}\:={AD}\mathrm{sin}\:\angle{DAF} \\ $$$$\:\:\:\:\:\:\:\:=\mathrm{cot}\:\theta×\frac{\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta}{\sqrt{\mathrm{1}+\left(\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta\right)^{\mathrm{2}} }} \\ $$$$\angle{BCE}\:=\frac{\pi}{\mathrm{4}}−\theta \\ $$$$\:\:\:\:{CE}\:={BE}\mathrm{cot}\:\left(\frac{\pi}{\mathrm{4}}−\theta\right) \\ $$$$\:\:\:\:\:\:\:\:\:\:\:\:\:=\frac{\mathrm{sin}\:\theta}{\mathrm{tan}\:\left(\frac{\pi}{\mathrm{4}}−\theta\right)} \\ $$$$\:\:{Given}\:{CE}\:=\:{FD} \\ $$$$\Rightarrow\:\frac{\mathrm{sin}\:\theta}{\mathrm{tan}\:\left(\frac{\pi}{\mathrm{4}}−\theta\right)}=\mathrm{cot}\:\theta×\frac{\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta}{\sqrt{\mathrm{1}+\left(\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta\right)^{\mathrm{2}} }} \\ $$$$\Rightarrow\:\frac{\mathrm{sin}\:\theta\left(\mathrm{1}+\mathrm{tan}\:\theta\right)\mathrm{tan}\:\theta}{\mathrm{1}−\mathrm{tan}\:\theta}=\frac{\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta}{\sqrt{\mathrm{1}+\left(\mathrm{1}+\mathrm{tan}\:\theta−\mathrm{cot}\:\theta\right)^{\mathrm{2}} }} \\ $$$${let}\:\:\mathrm{tan}\:\theta={t}\:\:\Rightarrow\:\:\mathrm{sin}\:\theta\:=\:\frac{{t}}{\sqrt{\mathrm{1}+{t}^{\mathrm{2}} }} \\ $$$$\Rightarrow\:\frac{{t}\left(\mathrm{1}+{t}\right){t}}{\sqrt{\mathrm{1}+{t}^{\mathrm{2}} }\left(\mathrm{1}−{t}\right)}=\frac{\mathrm{1}+{t}−\frac{\mathrm{1}}{{t}}}{\sqrt{\mathrm{1}+\left(\mathrm{1}+{t}−\frac{\mathrm{1}}{{t}}\right)^{\mathrm{2}} }} \\ $$$$\Rightarrow\:\frac{{t}^{\mathrm{4}} \left(\mathrm{1}+{t}\right)^{\mathrm{2}} }{\left(\mathrm{1}+{t}^{\mathrm{2}} \right)\left(\mathrm{1}−{t}\right)^{\mathrm{2}} }=\frac{\left({t}+{t}^{\mathrm{2}} −\mathrm{1}\right)^{\mathrm{2}} }{{t}^{\mathrm{2}} +\left({t}+{t}^{\mathrm{2}} −\mathrm{1}\right)^{\mathrm{2}} } \\ $$$$\Rightarrow\:{t}=\mathrm{tan}\:\theta\:\approx\:\mathrm{0}.\mathrm{63923} \\ $$$$\:\:\:\:\:\:\theta\:\approx\:\mathrm{32}.\mathrm{588}°\:. \\ $$

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