Let at the moment of the jump mr.X has the following speeds: \text{Let at the moment of the jump mr.X has the following speeds:} Let at the moment of the jump mr.X has the following speeds:
v x − instantaneous speed of movement horizontally v_x - \text{instantaneous speed of movement horizontally } v x − instantaneous speed of movement horizontally
v y − instantaneous vertical speed v_y - \text{instantaneous vertical speed} v y − instantaneous vertical speed
Then the coordinates mr.X will be: \text{Then the coordinates mr.X will be:} Then the coordinates mr.X will be:
x = v x t ( 1 ) x = v_xt(1) x = v x t ( 1 )
y = v y t − g t 2 2 ( 2 ) y = v_yt -\frac{gt^2}{2}(2) y = v y t − 2 g t 2 ( 2 )
The equations (1) and (2) coincide with the parametric \text{The equations (1) and (2) coincide with the parametric} The equations (1) and (2) coincide with the parametric
equations of a body thrown at an angle to the horizon. \text{ equations of a body thrown at an angle to the horizon.} equations of a body thrown at an angle to the horizon.
Where: \text{Where:} Where:
v = v x 2 + v y 2 -body speed v=\sqrt{v_x^2+v_y^2} \text{ -body speed} v = v x 2 + v y 2 -body speed
tan α = v y v x ; α − throw angle \tan \alpha= \frac{v_y}{v_x};\alpha-\text{throw angle} tan α = v x v y ; α − throw angle
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