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MOTION OF PROJECTILE

To analyze the projectile motion we use the following concept “Resolution of two dimensional motion into two one dimension motion” as discussed earlier. Hence it is easier to analyze the motion of projectile as composed of two simultaneous rectilinear motions which are independent of each other:

along the vertical y-axis with a uniform downward acceleration ‘g’ and

  • along the horizontal x-axis with a uniform velocity forward.

Consider a particle projected with an initial velocity u at an angle α with the horizontal x-axis as shown in figure 2.17. Velocity and accelerations can be resolved into two components:

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Velocity along x-axis = ux = u cos α

Acceleration along x-axis ax = 0

Velocity along y-axis = uy = u sin α

Acceleration along y-axis ay = -g

Here we use different equation of motions of one dimension derived earlier to get the different parameters.

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v2 = v02 – 2g (y – y0)                                …(C)

Total Time of flight

When body returns to the same horizontal level, the resultant displacement in vertical y-direction is zero. Use equation B.

Therefore,             0 = (u sin α) t – (½)gt2

or                   t = 2uSinα / g

(as t cannot equal to 0)

Horizontal Range

Horizontal Range (OA)  = Horizontal velocity × Time of flight

=        u cos α × 2u sin α/g

= u² sin 2α/g

=

Maximum Height

At the highest point of the trajectory, vertical component of velocity is zero.

Therefore              0 = (u sin α)2 – 2g Hmax

or,           Hmax = u² sin² α/ 2g

Equation of trajectory

Assuming the point of projection as the origin of co-ordinates and horizontal direction as the x-axis and vertical direction as the y-axis. Let P (x, y) be the position of the particle at instant after t second.

Then x = u cos α.t                and         y = u sin α.t – 1/2 gt²

Eliminating  ‘t’ form the above equations, we get,

y = x tan α – gx²/ 2u² cos² α

This is the equation of trajectory which is a parabola  (y = ax + bx2).

Illustrations

1.      A gun moving at a speed of 30m/sec fires at an angle 300 with a velocity 150m/s relative to the gun. Find the distance between the gun and the projectile when projectile hits the ground . (g = 10 m/sec)

Sol. Vertical component of velocity = 150 sin 300 = 75 m/sec

Horizontal component of velocity relative to gun = 150 cos 300

=                       =   75 √3 m/sec

Horizontal component of velocity relative to ground

=                              = 75 √3 + 30 ≈ 160 m/sec

Time of flight = (2 * 75 )/g = 15 sec

Range of projectile              = 160 × 15 = 2400 m

Distance moved by the gun and projectile = 2400 – 450 = 1950 m.

Consider a particle projected horizontally with a velocity u  from a point O as shown in figure 2.18.

Assuming the point of projection O as the origin of coordinates and horizontal direction as the X-axis and vertical direction as Y-axis. Let P (x, y) be the position of the particle after t seconds.

x = horizontal distance covered in time t = ut. …(1)

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y = vertical distance covered in time t  = ½gt2 ….(2)

Eliminate t from equations  (1) and (2) then

We get, y = (1/2 ) (g/u²) x²

This is the equation of parabola passing through the origin, with its vertex at the origin O. Hence the trajectory is a parabola.

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