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An airplane flies at a constant height h and constant speed j. A gun is at the origin (0,0). A shell is fired from the gun with an initial muzzle velocity v at an angle theta with the horizontal. What

Physics

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The correct option is C. v=(j2+2gh)1/2v = (j^2 + 2gh)^{1/2}.

Step 1: Define the motion of the airplane and the shell.
Let the gun be at the origin (0,0)(0,0).
The airplane flies at a constant height hh and constant speed jj. At time tt, its position is (xA,yA)=(jt,h)(x_A, y_A) = (jt, h).
The shell is fired with an initial muzzle velocity vv at an angle θ\theta with the horizontal. At time tt, its position is (xS,yS)(x_S, y_S).
The horizontal component of the shell's initial velocity is vx=vcos⁡θv_x = v \cos\theta.
The vertical component of the shell's initial velocity is vy=vsin⁡θv_y = v \sin\theta.
The equations of motion for the shell are:

xS(t)=(vcos⁡θ)tx_S(t) = (v \cos\theta) t yS(t)=(vsin⁡θ)t−12gt2y_S(t) = (v \sin\theta) t - \frac{1}{2} g t^2

Step 2: Set the conditions for the shell to hit the airplane.
For the shell to hit the airplane at time tt, their positions must be equal:

xS(t)=xA(t)  ⟹  (vcos⁡θ)t=jtx_S(t) = x_A(t) \implies (v \cos\theta) t = j t

Since t≠0t \neq 0 (the shell takes time to reach the airplane), we can divide by tt:

vcos⁡θ=j(∗)v \cos\theta = j \quad (*) yS(t)=yA(t)  ⟹  (vsin⁡θ)t−12gt2=h(∗∗)y_S(t) = y_A(t) \implies (v \sin\theta) t - \frac{1}{2} g t^2 = h \quad (**)

Step 3: Express sin⁡θ\sin\theta in terms of vv and jj.
From (∗)(*), cos⁡θ=jv\cos\theta = \frac{j}{v}.
Using the identity sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1:

sin⁡θ=1−cos⁡2θ=1−(jv)2=v2−j2v2=v2−j2v\sin\theta = \sqrt{1 - \cos^2\theta} = \sqrt{1 - \left(\frac{j}{v}\right)^2} = \sqrt{\frac{v^2 - j^2}{v^2}} = \frac{\sqrt{v^2 - j^2}}{v}

Step 4: Substitute sin⁡θ\sin\theta into equation (∗∗)(**) and solve for tt.
Substitute sin⁡θ\sin\theta into (∗∗)(**):

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