During the collision, the component of the velocity
∥ to the wall remains unchanged.
⇒ Let ⟶u be the velocity before collision and ⟶v be the velocity after collision.
The difference between ⟶u and ⟶v will always remain ⊥ normal to the wall canceling the components along the wall.
Let ∧n=α∧i+β∧j,(α2+β2=1), be the unit vector
Also, ⟶v−⟶u=((⟶v−⟶u)∧n)∧n
⟶v=4∧i−∧j ⟶u=∧i+3∧j
∴α=−35,β=45[∵α2+β2=1]
So, we get
∧n=−35∧i+45∧j
We know that,
Coefficient of restitution,
e=−⟶v∧n⟶u∧n=−(−3)+12−12−4=916
∴n16=916
⇒n=9.