Question #49907

A rock is thrown at a window that is located 18m above the ground. The rock is thrown at an angle 40 degrees above the horizontal. The rock is thrown from a height of 2.00m above the ground with a speed of 30m/s and experiences no appreciable air resistance. If the rock strikes the window on its upward trajectory, from what horizontal distance from the window was it released???
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Expert's answer

2014-12-09T01:56:39-0500

Answer on Question#49708 – Physics – Mechanics | Kinematics | Dynamics


L=30cos(40)×(3sin(40)9sin2(40)165)27.77L = 30 \cos (40{}^{\circ}) \times \left(3 \sin (40{}^{\circ}) - \sqrt{9 \sin^{2} (40{}^{\circ}) - \frac{16}{5}}\right) \approx 27.77


Solution



Equations of motion:


md2xdt2=0m \frac{d^{2} x}{d t^{2}} = 0md2ydt2=mgm \frac{d^{2} y}{d t^{2}} = - m g


Initial conditions:


x=0;Vx(0)=30cos(40);y(0)=2;Vy(0)=30sin(40);x = 0; \quad V_{x}(0) = 30 \cos (40{}^{\circ}); \quad y(0) = 2; \quad V_{y}(0) = 30 \sin (40{}^{\circ});


Explicit solutions of the equations above:


x=C1+C2tx = C_{1} + C_{2} ty=gt22+C3t+C4y = - \frac{g t^{2}}{2} + C_{3} t + C_{4}


Use initial conditions:


x(0)=C1+C2(0)=C1=0x(0) = C_1 + C_2(0) = C_1 = 0Vx(0)=dxdt(0)=C2=30cos(40)V_x(0) = \frac{dx}{dt}(0) = C_2 = 30 \cos(40{}^\circ)y(0)=g(0)22+C3(0)+C4=C4=2y(0) = -\frac{g(0)^2}{2} + C_3(0) + C_4 = C_4 = 2Vy(0)=dydt(0)=g(0)+C3=C3=30sin(40)V_y(0) = \frac{dy}{dt}(0) = -g(0) + C_3 = C_3 = 30 \sin(40{}^\circ)


Thus, we have:


x(t)=30cos(40)tx(t) = 30 \cos(40{}^\circ) ty(t)=2+30sin(40)tgt22y(t) = 2 + 30 \sin(40{}^\circ) t - \frac{g t^2}{2}


Assume g=10g = 10

y(t)=2+30sin(40)t5t2y(t) = 2 + 30 \sin(40{}^\circ) t - 5 t^2


Our aim to define such distance LL that at some time t1t_1: y(t1)=18y(t_1) = 18; Vy(t1)0V_y(t_1) \geq 0.


2+30sin(40)t15t12=182 + 30 \sin(40{}^\circ) t_1 - 5 t_1^2 = 185t12+30sin(40)t116=0-5 t_1^2 + 30 \sin(40{}^\circ) t_1 - 16 = 0t126sin(40)t1+165=0t_1^2 - 6 \sin(40{}^\circ) t_1 + \frac{16}{5} = 0D=36sin2(40)645D = 36 \sin^2(40{}^\circ) - \frac{64}{5}t1()=6sin(40)+36sin2(40)6452=3sin(40)+9sin2(40)165t_1(\downarrow) = \frac{6 \sin(40{}^\circ) + \sqrt{36 \sin^2(40{}^\circ) - \frac{64}{5}}}{2} = 3 \sin(40{}^\circ) + \sqrt{9 \sin^2(40{}^\circ) - \frac{16}{5}}t1()=3sin(40)9sin2(40)165t_1(\uparrow) = 3 \sin(40{}^\circ) - \sqrt{9 \sin^2(40{}^\circ) - \frac{16}{5}}


Obviously, t1()t_1(\uparrow) refers to upward trajectory, t1()t_1(\downarrow) – downward trajectory.

Determine L=x(t1)L = x(t_1)

L=30cos(40)×(3sin(40)9sin2(40)165)27.77L = 30 \cos(40{}^\circ) \times \left(3 \sin(40{}^\circ) - \sqrt{9 \sin^2(40{}^\circ) - \frac{16}{5}}\right) \approx 27.77


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