BdPhO Regional (Dhaka-South) Secondary 2019/7
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$C$ is the point on ground straight down to point $B$.
How far from the point $C$ does Azmain fall on the ground?
$The$ $only$ $way$ $to$ $learn$ $mathematics$ $is$ $to$ $do$ $mathematics$. $-$ $PAUL$ $HALMOS$
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Re: BdPhO Regional (Dhaka-South) Secondary 2019/7
Let the point where the water slide touches the ground be $D$. At point $D$, $v_0^2=2gH$.
At point $B$, $v^2=v_0^2-2gh=2g(H-h)$.
Now, Azmain should travel on PROJECTILE MOTION.(If you have no idea about projectile motion, you can click on the link for easy explanation.)
Velocity among $X$ axis, $v_x=vcosθ$.
Velocity among $Y$ axis, $v_y=vsinθ$.
Now, total time required, $t=t_1+t_2=\dfrac{2vsinθ}{g}+\dfrac{\sqrt{v^2sin^2θ+2gh}-vsinθ}{g}=\dfrac{vsinθ+\sqrt{v^2sin^2θ+2gh}}{g}$
So, distance from point $C$,
$d=v_xt=vcosθ\dfrac{vsinθ+\sqrt{v^2sin^2θ+2gh}}{g}=\sqrt{2g(H-h)}cosθ\dfrac{\sqrt{2g(H-h)}sinθ+\sqrt{2g(H-h)sin^2θ+2gh}}{g}=\dfrac{2g(H-h)cosθ sinθ+\sqrt{4g^2(H-h)^2sin^2θ cos^2θ+4g^2(H-h)h cos^2θ}}{g}=\dfrac{2g(H-h)cosθ sinθ+2g\sqrt{(H-h)^2sin^2θ cos^2θ+(H-h)h cos^2θ}}{g}=2\left((H-h)cosθ sinθ+\sqrt{(H-h)^2sin^2θ cos^2θ+(H-h)h cos^2θ}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)^2sin^2θ +(H-h)h}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ-hsin^2θ +h)}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ+h(1-sin^2θ))}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ+h cos^2θ)}\right)$
The interesting fact is that distance of the system doesn't depend on gravity. That means, Azmain would travel same distance in both the Earth and the moon, if there was no wind resistance.
At point $B$, $v^2=v_0^2-2gh=2g(H-h)$.
Now, Azmain should travel on PROJECTILE MOTION.(If you have no idea about projectile motion, you can click on the link for easy explanation.)
Velocity among $X$ axis, $v_x=vcosθ$.
Velocity among $Y$ axis, $v_y=vsinθ$.
Now, total time required, $t=t_1+t_2=\dfrac{2vsinθ}{g}+\dfrac{\sqrt{v^2sin^2θ+2gh}-vsinθ}{g}=\dfrac{vsinθ+\sqrt{v^2sin^2θ+2gh}}{g}$
So, distance from point $C$,
$d=v_xt=vcosθ\dfrac{vsinθ+\sqrt{v^2sin^2θ+2gh}}{g}=\sqrt{2g(H-h)}cosθ\dfrac{\sqrt{2g(H-h)}sinθ+\sqrt{2g(H-h)sin^2θ+2gh}}{g}=\dfrac{2g(H-h)cosθ sinθ+\sqrt{4g^2(H-h)^2sin^2θ cos^2θ+4g^2(H-h)h cos^2θ}}{g}=\dfrac{2g(H-h)cosθ sinθ+2g\sqrt{(H-h)^2sin^2θ cos^2θ+(H-h)h cos^2θ}}{g}=2\left((H-h)cosθ sinθ+\sqrt{(H-h)^2sin^2θ cos^2θ+(H-h)h cos^2θ}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)^2sin^2θ +(H-h)h}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ-hsin^2θ +h)}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ+h(1-sin^2θ))}\right)=2cosθ\left((H-h) sinθ+\sqrt{(H-h)(H sin^2θ+h cos^2θ)}\right)$
The interesting fact is that distance of the system doesn't depend on gravity. That means, Azmain would travel same distance in both the Earth and the moon, if there was no wind resistance.
$The$ $only$ $way$ $to$ $learn$ $mathematics$ $is$ $to$ $do$ $mathematics$. $-$ $PAUL$ $HALMOS$