Answer on Question#49708 – Physics – Mechanics | Kinematics | Dynamics
L = 30 cos ( 40 ∘ ) × ( 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 16 5 ) ≈ 27.77 L = 30 \cos (40{}^{\circ}) \times \left(3 \sin (40{}^{\circ}) - \sqrt{9 \sin^{2} (40{}^{\circ}) - \frac{16}{5}}\right) \approx 27.77 L = 30 cos ( 40 ∘ ) × ( 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 5 16 ) ≈ 27.77
Solution
Equations of motion:
m d 2 x d t 2 = 0 m \frac{d^{2} x}{d t^{2}} = 0 m d t 2 d 2 x = 0 m d 2 y d t 2 = − m g m \frac{d^{2} y}{d t^{2}} = - m g m d t 2 d 2 y = − m g
Initial conditions:
x = 0 ; V x ( 0 ) = 30 cos ( 40 ∘ ) ; y ( 0 ) = 2 ; V y ( 0 ) = 30 sin ( 40 ∘ ) ; x = 0; \quad V_{x}(0) = 30 \cos (40{}^{\circ}); \quad y(0) = 2; \quad V_{y}(0) = 30 \sin (40{}^{\circ}); x = 0 ; V x ( 0 ) = 30 cos ( 40 ∘ ) ; y ( 0 ) = 2 ; V y ( 0 ) = 30 sin ( 40 ∘ ) ;
Explicit solutions of the equations above:
x = C 1 + C 2 t x = C_{1} + C_{2} t x = C 1 + C 2 t y = − g t 2 2 + C 3 t + C 4 y = - \frac{g t^{2}}{2} + C_{3} t + C_{4} y = − 2 g t 2 + C 3 t + C 4
Use initial conditions:
x ( 0 ) = C 1 + C 2 ( 0 ) = C 1 = 0 x(0) = C_1 + C_2(0) = C_1 = 0 x ( 0 ) = C 1 + C 2 ( 0 ) = C 1 = 0 V x ( 0 ) = d x d t ( 0 ) = C 2 = 30 cos ( 40 ∘ ) V_x(0) = \frac{dx}{dt}(0) = C_2 = 30 \cos(40{}^\circ) V x ( 0 ) = d t d x ( 0 ) = C 2 = 30 cos ( 40 ∘ ) y ( 0 ) = − g ( 0 ) 2 2 + C 3 ( 0 ) + C 4 = C 4 = 2 y(0) = -\frac{g(0)^2}{2} + C_3(0) + C_4 = C_4 = 2 y ( 0 ) = − 2 g ( 0 ) 2 + C 3 ( 0 ) + C 4 = C 4 = 2 V y ( 0 ) = d y d t ( 0 ) = − g ( 0 ) + C 3 = C 3 = 30 sin ( 40 ∘ ) V_y(0) = \frac{dy}{dt}(0) = -g(0) + C_3 = C_3 = 30 \sin(40{}^\circ) V y ( 0 ) = d t d y ( 0 ) = − g ( 0 ) + C 3 = C 3 = 30 sin ( 40 ∘ )
Thus, we have:
x ( t ) = 30 cos ( 40 ∘ ) t x(t) = 30 \cos(40{}^\circ) t x ( t ) = 30 cos ( 40 ∘ ) t y ( t ) = 2 + 30 sin ( 40 ∘ ) t − g t 2 2 y(t) = 2 + 30 \sin(40{}^\circ) t - \frac{g t^2}{2} y ( t ) = 2 + 30 sin ( 40 ∘ ) t − 2 g t 2
Assume g = 10 g = 10 g = 10
y ( t ) = 2 + 30 sin ( 40 ∘ ) t − 5 t 2 y(t) = 2 + 30 \sin(40{}^\circ) t - 5 t^2 y ( t ) = 2 + 30 sin ( 40 ∘ ) t − 5 t 2
Our aim to define such distance L L L that at some time t 1 t_1 t 1 : y ( t 1 ) = 18 y(t_1) = 18 y ( t 1 ) = 18 ; V y ( t 1 ) ≥ 0 V_y(t_1) \geq 0 V y ( t 1 ) ≥ 0 .
2 + 30 sin ( 40 ∘ ) t 1 − 5 t 1 2 = 18 2 + 30 \sin(40{}^\circ) t_1 - 5 t_1^2 = 18 2 + 30 sin ( 40 ∘ ) t 1 − 5 t 1 2 = 18 − 5 t 1 2 + 30 sin ( 40 ∘ ) t 1 − 16 = 0 -5 t_1^2 + 30 \sin(40{}^\circ) t_1 - 16 = 0 − 5 t 1 2 + 30 sin ( 40 ∘ ) t 1 − 16 = 0 t 1 2 − 6 sin ( 40 ∘ ) t 1 + 16 5 = 0 t_1^2 - 6 \sin(40{}^\circ) t_1 + \frac{16}{5} = 0 t 1 2 − 6 sin ( 40 ∘ ) t 1 + 5 16 = 0 D = 36 sin 2 ( 40 ∘ ) − 64 5 D = 36 \sin^2(40{}^\circ) - \frac{64}{5} D = 36 sin 2 ( 40 ∘ ) − 5 64 t 1 ( ↓ ) = 6 sin ( 40 ∘ ) + 36 sin 2 ( 40 ∘ ) − 64 5 2 = 3 sin ( 40 ∘ ) + 9 sin 2 ( 40 ∘ ) − 16 5 t_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}} t 1 ( ↓ ) = 2 6 sin ( 40 ∘ ) + 36 sin 2 ( 40 ∘ ) − 5 64 = 3 sin ( 40 ∘ ) + 9 sin 2 ( 40 ∘ ) − 5 16 t 1 ( ↑ ) = 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 16 5 t_1(\uparrow) = 3 \sin(40{}^\circ) - \sqrt{9 \sin^2(40{}^\circ) - \frac{16}{5}} t 1 ( ↑ ) = 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 5 16
Obviously, t 1 ( ↑ ) t_1(\uparrow) t 1 ( ↑ ) refers to upward trajectory, t 1 ( ↓ ) t_1(\downarrow) t 1 ( ↓ ) – downward trajectory.
Determine L = x ( t 1 ) L = x(t_1) L = x ( t 1 )
L = 30 cos ( 40 ∘ ) × ( 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 16 5 ) ≈ 27.77 L = 30 \cos(40{}^\circ) \times \left(3 \sin(40{}^\circ) - \sqrt{9 \sin^2(40{}^\circ) - \frac{16}{5}}\right) \approx 27.77 L = 30 cos ( 40 ∘ ) × ( 3 sin ( 40 ∘ ) − 9 sin 2 ( 40 ∘ ) − 5 16 ) ≈ 27.77
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