A 10 ft plank is leaning against a wall. If at a certain instant the bottom of the plank is 2 ft from the wall and is being pushed toward the wall at the rate of 6 in/s , how fast is the acute angle that the plank makes with the ground increasing?
Solution:
dxdt=−6 in/sec=−0.5 ft/sec ...(i)dθdt=?cosθ=x10\dfrac{dx}{dt}=-6\ in/sec=-0.5\ ft/sec\ ...(i) \\ \dfrac{d \theta}{dt}=? \\ \cos \theta=\dfrac{x}{10}dtdx=−6 in/sec=−0.5 ft/sec ...(i)dtdθ=?cosθ=10x
On differentiating both sides w.r.t ttt,
−sinθdθdt=110dxdt-\sin \theta \dfrac{d \theta}{dt} =\dfrac1{10}\dfrac{dx}{dt}−sinθdtdθ=101dtdx ...(ii)
Using pythagoras theorem,
h2+x2=102h^2 +x^2 =10^2h2+x2=102
When x=2x=2x=2
h2+22=102⇒h2=100−4=96⇒h=96=46 fth^2 +2^2 =10^2 \\ \Rightarrow h^2 =100-4=96 \\ \Rightarrow h=\sqrt{96}=4\sqrt 6\ fth2+22=102⇒h2=100−4=96⇒h=96=46 ft
Now, sinθ=h10=4610=265\sin \theta=\dfrac{h}{10}=\dfrac{4\sqrt6}{10}=\dfrac{2\sqrt6}{5}sinθ=10h=1046=526 ...(iii)
Using (i) and (iii) in (ii),
−(265)dθdt=110×(−0.5)⇒dθdt=0.051 rad/sec-(\dfrac{2\sqrt6}{5}) \dfrac{d \theta}{dt} =\dfrac1{10}\times (-0.5) \\ \Rightarrow \dfrac{d \theta}{dt}=0.051\ rad/sec−(526)dtdθ=101×(−0.5)⇒dtdθ=0.051 rad/sec
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