Question
Question: Assume that every projectile fired by the toy cannon experiences a constant net force F along the en...
Assume that every projectile fired by the toy cannon experiences a constant net force F along the entire length of barrel. If a projectile of mass m leaves the barrel of the cannon with a speed v, at what speed will a projectile of mass 2m leave the barrel?
A. 2v
B. 2v
C. v
D. 2v
E. 4v
Solution
n physics, projectile is the motion of a body when given a certain force and it follows a particular trajectory. Here, we will use the general formulas of force on a body which is defined as the product of mass of the body and its acceleration, mathematically written as F=ma and we will use the newton’s equation of motion as v2−u2=2aS where, v is the final velocity along the distance S and u is the acceleration of the body.
Complete step by step answer:
Let us suppose F be the net force acting on both bodies of mass m(and)2m , let their accelerations be am(and)a2m respectively, so using
F=ma We have,
⇒F=mam
And
F=2ma2m
Since both forces are equal so we write
mam=2ma2m
⇒a2mam=2→(i)
Now for the length of L mass m leaves with velocity v with an acceleration of am and having initial velocity of u=0 so by using, v2−u2=2aS we can write,
v2−0=2amL
⇒v2=2amL
Similarly, for the length of L mass 2m leaves with velocity say v′ with an acceleration of a2m and having initial velocity of u=0 so by using, v2−u2=2aS we can write,
v′2−0=2a2mL
⇒v′2=2a2mL
Now, divide the equation v′2=2a2mL by the equation v2=2amL we get,
v2v′2=ama2m
From the equation (i) put ama2m=21
v′2=v2×21
∴v′=2v
So, the mass 2m body leaves the barrel with a velocity of v′=2v.
Hence, the correct option is B.
Note: It should be remembered that, while using the newton’s equation of motion v2−u2=2aS , the initial velocity of the projectile body when enters in a barrel is taken as zero and other equation of motion are written as v=u+at and S=ut+21at2 ,these equations of motion is widely used in classical kinematics to deal with physical problems of physics.