Case II Projection in upward direction with some angle with horizonta
Vertical mirror
sign convention
Horizontal Mirror
x = (u cosq) t
Case III Projection in downward direction with some angle with horizontal
Vertical Mirror
Horizontal Mirror
Projectile along inclined plane For Simplicity & understanding
Vertical Mirror
V = u - g t
O = u sin b - (g cosa) t
Horizontal Mirror
OB = OA Cos a
Special case of Projectile Motion
Case I
(i) Time of flight let OQ ® x -axis
OP ® y –axis
ux = u
uy = 0
ax = - g sin b
ay = - g cos b
Now
Vx = ux + axt
O = u – g sin bt
(ii) Final velocity V
Vy = uy + ay t
V = 0 – g cos b
V = u cot b
(iii) Height h
Now
h = Sy sin a
(iv) Distance AB
Now
Case 2
(i) Time after which V1 ^ V2
Ball 1
Ball 2
Now
g2 t2 = u1 u2
(ii) gap between the ball 1 and ball 2 at the time
Ball 1 x1 = u1 t,
Ball 2
x2 = - u2t
Gap between Ball 1 and Ball 2
Gap = (u1 + u2) t
Case 3 Collision of two projectile
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