Correct Answer - `t_(0)=12sec,v=100sqrt3//11`
(a) `100m//s` velocity of the ball is relative to ground
[Unless and until it is mentioned in the question, the velocity is always relative to ground]
Horizontal component of velocity of cannon ball,
`u_(x)=ucos30^(@)`
or `u_(x)=(100)xx(sqrt3)/(2)=50sqrt3m//s`
and vertical component `o` its velocity
`u_(y)=usin30^(@)`
`u_(y)=100xx(1)/(2)=50m//s`
and vertical displacement of the ball when it strike the carriage is `-120m` or
`s_(y)=u_(y)t+(1)/(2)a_(y)t^(2)`
`rArr" "-120=(50t)+((1)/(2))(-10)t^(2)`
`rArr" "t^(2)-10t-24=0t=12"s or"-2s`
Ignoring the negative time, we have
(b) When it strikes the carriage, its horizontal component of velocity is still `50sqrt3m//s`. It strikes to the carriage. Let `v_(2)` be the velocity of (carriage+ball) system after collision. The applying conservation of linear momentum in horizontal direction
(mass of ball) (horizontal component of its velocity before collision)=(mass of ball+carrigage)(v_(2))`
` therefore" "(1 kg)(50sqrt3m//s)=(10 kg)(v_(2))`
`therefore" "v_(2)=5sqrt3m//s`
The second ball is fired when the first ball strikes the carrige i.e. after 12s. In these 12x the car will move forward a distance of `12v_(1)` or `60sqrt3m`.
The second ball also take 12s to travel a vertical displacment of `-120m`. This ball will strike the carriage `60sqrt3m` in these 12s. This is possible only when resistive carriage after first collision `(v_(2))=5sqrt3m//s`
Hence, at the time of second collision
Horizontal component of velocity of ball`=50sqrt3m//s` and horizontal velocity of carriage + first ball `= 5sqrt3m//s`. Let `v` be the disired velocity of carriage after second collision. Then conservation of lilnear momentum in horizontal direction gives
`11v=(1)(50sqrt3)+(10)(5sqrt3)=100sqrt3`
`therefore" "v=(100sqrt3)/(11)m//s` or `v=15.75m//s`
In this particular problem values are so adjusted that even it we that the velocity of ball with respect to car, we get the same results of both parts, although the method will be wrong.