Answer on Question#49946 - Physics - Mechanics | Kinematics | Dynamics
1. y ( V y 0 g ) = V y 0 2 2 g = 5 y\left(\frac{V_{y0}}{g}\right) = \frac{V_{y0}^2}{2g} = 5 y ( g V y 0 ) = 2 g V y 0 2 = 5
2. x ( 2 V y 0 g ) = V x 0 2 V y 0 g = 40 x\left(\frac{2V_{y0}}{g}\right) = V_{x0} \frac{2V_{y0}}{g} = 40 x ( g 2 V y 0 ) = V x 0 g 2 V y 0 = 40
3. V = 10 5 V = 10\sqrt{5} V = 10 5 . Direction is reflection from the x-axis of initial velocity.
Solution
Equations of motion:
x ( t ) = V x 0 t + x 0 x (t) = V _ {x 0} t + x _ {0} x ( t ) = V x 0 t + x 0 y ( t ) = − g t 2 2 + V y 0 t + y 0 y (t) = - \frac {g t ^ {2}}{2} + V _ {y 0} t + y _ {0} y ( t ) = − 2 g t 2 + V y 0 t + y 0
Initial conditions:
x 0 = 0 x _ {0} = 0 x 0 = 0 y 0 = 0 y _ {0} = 0 y 0 = 0 V x 0 = 20 V _ {x 0} = 2 0 V x 0 = 20 V y 0 = 10 V _ {y 0} = 1 0 V y 0 = 10
Thus,
x ( t ) = V x 0 t x (t) = V _ {x 0} t x ( t ) = V x 0 t y ( t ) = − g t 2 2 + V y 0 t y (t) = - \frac {g t ^ {2}}{2} + V _ {y 0} t y ( t ) = − 2 g t 2 + V y 0 t
1) the maximum height of the particle
It's value of y ( t ) y(t) y ( t ) at time, when d y ( t ) d t = 0 \frac{dy(t)}{dt} = 0 d t d y ( t ) = 0 .
d y ( y ) d t = − g t + V y 0 = 0 \frac{dy(y)}{dt} = -gt + V_{y0} = 0 d t d y ( y ) = − g t + V y 0 = 0 t = V y 0 g t = \frac{V_{y0}}{g} t = g V y 0 y ( V y 0 g ) = − g ( V y 0 g ) 2 2 + V y 0 ( V y 0 g ) = V y 0 2 2 g y \left(\frac{V_{y0}}{g}\right) = - \frac{g \left(\frac{V_{y0}}{g}\right)^2}{2} + V_{y0} \left(\frac{V_{y0}}{g}\right) = \frac{V_{y0}^2}{2g} y ( g V y 0 ) = − 2 g ( g V y 0 ) 2 + V y 0 ( g V y 0 ) = 2 g V y 0 2
Substitute V y 0 = 10 V_{y0} = 10 V y 0 = 10 ; g = 10 g = 10 g = 10 .
y ( V y 0 g ) = y ( 1 ) = 1 0 2 2 × 10 = 5 y \left(\frac{V_{y0}}{g}\right) = y(1) = \frac{10^2}{2 \times 10} = 5 y ( g V y 0 ) = y ( 1 ) = 2 × 10 1 0 2 = 5
2) the horizontal distance from the point of projection when it returns to the ground.
"Returns to ground" ≡ y ( t ) = 0 , t ≠ 0 \equiv y(t) = 0, t \neq 0 ≡ y ( t ) = 0 , t = 0 .
y ( t ) = − g t 2 2 + V y 0 t = t ( − g t 2 + V y 0 ) = 0 y(t) = - \frac{g t^2}{2} + V_{y0} t = t \left(- \frac{g t}{2} + V_{y0}\right) = 0 y ( t ) = − 2 g t 2 + V y 0 t = t ( − 2 g t + V y 0 ) = 0 t = 2 V y 0 g t = \frac{2 V_{y0}}{g} t = g 2 V y 0 x ( 2 V y 0 g ) = V x 0 2 V y 0 g x \left(\frac{2 V_{y0}}{g}\right) = V_{x0} \frac{2 V_{y0}}{g} x ( g 2 V y 0 ) = V x 0 g 2 V y 0
Substitute V x 0 = 20 V_{x0} = 20 V x 0 = 20 ; V y 0 = 10 V_{y0} = 10 V y 0 = 10 ; g = 10 g = 10 g = 10 .
x ( 2 V y 0 g ) = x ( 2 ) = 20 × 2 = 40 x \left(\frac{2 V_{y0}}{g}\right) = x(2) = 20 \times 2 = 40 x ( g 2 V y 0 ) = x ( 2 ) = 20 × 2 = 40
3) the magnitude and direction of its velocity on landing.
d y d t ( 2 V y 0 g ) = − g ( 2 V y 0 g ) + V y 0 = − V y 0 \frac{dy}{dt} \left(\frac{2 V_{y0}}{g}\right) = -g \left(\frac{2 V_{y0}}{g}\right) + V_{y0} = - V_{y0} d t d y ( g 2 V y 0 ) = − g ( g 2 V y 0 ) + V y 0 = − V y 0 d x d t ( 2 V y 0 g ) = V x 0 \frac{dx}{dt} \left(\frac{2 V_{y0}}{g}\right) = V_{x0} d t d x ( g 2 V y 0 ) = V x 0
Hence, magnitude still the same
V = V x 0 2 + V y 0 2 = 2 0 2 + 1 0 2 = 400 + 100 = 500 = 10 5 V = \sqrt{V_{x0}^2 + V_{y0}^2} = \sqrt{20^2 + 10^2} = \sqrt{400 + 100} = \sqrt{500} = 10\sqrt{5} V = V x 0 2 + V y 0 2 = 2 0 2 + 1 0 2 = 400 + 100 = 500 = 10 5
Direction is reflection from the x-axis of initial velocity.
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