Horizontal motion
The horizontal component of the velocity v x remains unchanged throughout the motion.
v x = v 0 x = v 0 c o s Ï‘ 0 = c o n s t [
] , where:
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
Horizontal displacement
Horizontal displacement is described by the formula:
x ( t ) = x 0 + v 0 x t
x ( t ) = x 0 + ( v 0 c o s Ï‘ 0 ) t [m], where:
x 0 - initial position
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
t - time
Vertical motion
The vertical component of the velocity v y increases linearly, because the acceleration due to gravity g is constant.
v y = v 0 y − g t =v 0 s i n Ï‘ 0 − g t [
] , where:
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
t - time
g - acceleration due to gravity
Vertical displacement
Vertical displacement is described by the formula:
y ( t ) = y 0 + v 0 y t −
y ( t ) = y 0 + ( v 0 s i n Ï‘ 0 ) t −
[m], where:
x 0 - initial position
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
t - time
g - acceleration due to gravity
Trajectory
If we eliminate t between x ( t ) and y ( t ) equations we will obtain the following equation:
y = ( t g Ï‘ 0 ) x −
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
g - acceleration due to gravity
Range of a projectile time dependent
Assuming a flat Earth with a uniform gravity field, and no air resistance, a projectile launched with specific initial conditions will have a predictable range. This range time dependent is the total horizontal distance traveled by the projectile and can be described by the formula:
R ( t ) = ( v 0 c o s Ï‘ 0 ) t [m], where:
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
Range of a projectile time independent
Assuming a flat Earth with a uniform gravity field, and no air resistance, a projectile launched with specific initial conditions will have a predictable range. This range time independent is the total horizontal distance traveled by the projectile and can be described by the formula:
R =
s i n ( 2 Ï‘ 0 ) [m], where:
v 0 - initial velocity
Ï‘ 0 - launch angle - the angle between v 0 and positive direction of the x axis
g - acceleration due to gravity
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