The given situation can be represented as shown in the following figure.
Where,
\(AO\) = Incident path of the ball
\(OB\) = Path followed by the ball after deflection
\(\angle\)\(AOB\) = Angle between the incident and deflected paths of the ball = \(45\degree\)
\(\angle AOP\) = \(\angle BOP\) = \(22.5\degree\) = \(θ\)
Initial and final velocities of the ball = \(v\)
Horizontal component of the initial velocity = \(v\cos \theta\) along \(RO\)
Vertical component of the initial velocity = \(v\sin \theta\) along \(PO\)
Horizontal component of the final velocity = \(v\cos \theta\) along \(OS\)
Vertical component of the final velocity = \(v\sin \theta\) along \(OP\)
The horizontal components of velocities suffer no change. The vertical components of velocities are in the opposite directions.
\(\therefore\) Impulse imparted to the ball = Change in the linear momentum of the ball
= \(mv \cos \theta - (-\;mv \cos \theta)\)
= \(2mv \cos \theta\)
Mass of the ball, \(m\) = \(0.15 \;kg\)
Velocity of the ball, \(v\) = \(54\; km/h\) = \(15 \;m/s\)
\(\therefore\) Impulse = \(2 × 0.15 × 15 \cos 22.5\degree\)
= \(4.16 \;kg \;m/s\)
Newton’s 1st law states that a body at rest or uniform motion will continue to be at rest or uniform motion until and unless a net external force acts on it.
Newton’s 2nd law states that the acceleration of an object as produced by a net force is directly proportional to the magnitude of the net force, in the same direction as the net force, and inversely proportional to the object’s mass.
Mathematically, we express the second law of motion as follows:
Newton’s 3rd law states that there is an equal and opposite reaction for every action.