Question
Question: An open watertight railway wagon of mass \[5\times {{10}^{3}}\,kg\]coasts at an initial velocity of ...
An open watertight railway wagon of mass 5×103kgcoasts at an initial velocity of 1.2m/swithout friction on a railway track. Rain falls vertically downwards into the wagon. What change then occurred in the kinetic energy of the wagon, when it has collected 103kg water?
(A) 1200J
(B) 300J
(C) 600J
(D) 900J
Solution
Hint : In this question, we have the value of the mass of the wagon and its velocity along with a mass of water. We are required to find the change in kinetic energy of the wagon and in order to find that we will use the formula of momentum and kinetic energy.
Complete step by step answer:
Given:
Mass of railway wagon =5×103kg
Initial velocity =1.2m/s
Mass of water =103kg
Change in kinetic energy of the wagon =?
Since force in the horizontal direction=0,
Pi=Pf.....(1)
Where,
Pi= Initial momentum
Pf= Final momentum
Momentum is defined as the product of a system’s mass multiplied by its velocity,
P=m×v
Where,
P=Momentum
m=Mass
v=Velocity
Initial momentum (Pi) will be the sum of the momentum of the wagon and momentum of the water. Whereas, Final momentum will be equal to the sum of the mass of water and wagon multiplied by velocity.
Since the velocity of water is equal to 0,
Therefore,
(5×103×1.2)+(103×0)=(6×103)v
6×103=(6×103)v
v=1m/s
To find the change in kinetic energy, we will find the final and initial kinetic energy.
Final kinetic energy,
(KE)f=21mfvf2
Where,
mf= Final mass
vf= Final velocity
(KE)f=21(6×103×12)
(KE)f=3000J
Initial kinetic energy,
(KE)i=21mivi2
Where,
mi=Initial mass
vi=Initial velocity
(KE)i=21(5×103×(1.2)2)
(KE)i=3600J
As we know change in kinetic energy is:
ΔKE=(KE)i−(KE)f
ΔKE=3600−3000
ΔKE=600J
So the change in kinetic energy of the wagon is 600 J. Hence option C is correct.
Note: In order to solve this kind of question we should have knowledge about momentum and kinetic energy. The change in the kinetic energy of an object is equal to the net work done on the object. This fact is referred to as the Work-Energy Principle and is often a very useful tool in mechanics problem-solving.