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Question: A body of mass \(1Kg\), initially at rest, explodes and breaks into three fragments of masses in the...

A body of mass 1Kg1Kg, initially at rest, explodes and breaks into three fragments of masses in the ratio 1:1:31:1:3. The two pieces of equal mass fly off perpendicular to each other with a speed of 30ms130m{s^{ - 1}} each. What is the velocity of the heavier fragment?

Explanation

Solution

To solve this question, we should use the concept of conservation of linear momentum. We should always remember that the total or net momentum of a system is always conserved before and after any event.

Formulae used:
Law of conservation of momentum,
momentumbefore=momentumaftermomentu{m_{before}} = momentu{m_{after}}
Here momentumbeforemomentu{m_{before}} is the momentum of the system before explosion and
momentumaftermomentu{m_{after}} is the momentum of the system after an explosion.
p=mv\vec p = m\vec v
Here p\vec p is the momentum of the body, mm is the mass of the body and v\vec v is the velocity of the body.

Complete step by step answer:
In the question, it is given that the mass of the body was 1Kg1Kg and it exploded into three fragments.
Let the masses of individual fragments be m1{m_1}, m2{m_2} and m3{m_3}. It is given in the question that the masses are in the ratio 1:1:31:1:3. So the values of mass of each fragment is,
m1=1×15=0.2Kg{m_1} = 1 \times \dfrac{1}{5} = 0.2Kg,
m2=1×15=0.2Kg{m_2} = 1 \times \dfrac{1}{5} = 0.2Kg and
m3=1×35=0.6Kg{m_3} = 1 \times \dfrac{3}{5} = 0.6Kg.
We know that the momentum of the system is always conserved. So,
Mu=m1v1+m2v2+m3v3M\vec u = {m_1}{\vec v_1} + {m_2}{\vec v_2} + {m_3}{\vec v_3}
Here MM is the mass of the particle before explosion,
uu is the velocity of the particle before explosion,
m1{m_1}, m2{m_2} and m3{m_3} are the masses of the fragments after explosion and
v1{v_1}, v2{v_2} and v3{v_3} are the velocities of the fragments after the explosion.
We know that the body is at rest before explosion as it’s already given in the question. So,
u=0u = 0
0=m1v1+m2v2+m3v3\Rightarrow 0 = {m_1}{\vec v_1} + {m_2}{\vec v_2} + {m_3}{\vec v_3}
Substituting the values of m1{m_1}, m2{m_2} and m3{m_3} in the above equation, we get
0=0.2v1+0.2v2+0.6v3\Rightarrow 0 = 0.2{\vec v_1} + 0.2{\vec v_2} + 0.6{\vec v_3}
v1+v2=3v3\Rightarrow {\vec v_1} + {\vec v_2} = - 3{\vec v_3}
Let this be equation 1.
In the question, it is said that two of the particles with equal mass fly off perpendicular to each other with a speed of 30ms130m{s^{ - 1}} each.

The resultant of the velocities v1{v_1} and v2{v_2} will be
Vr=v1+v2\Rightarrow {\vec V_r} = {\vec v_1} + {\vec v_2}
Vr=v12+v22+v1v2cosθ=302+302+(30×30×cos90)=42.42ms1\Rightarrow {V_r} = \sqrt {v_1^2 + v_2^2 + {v_1}{v_2}\cos \theta } = \sqrt {{{30}^2} + {{30}^2} + \left( {30 \times 30 \times \cos 90^\circ } \right)} = 42.42m{s^{ - 1}}
Here Vr{\vec V_r} is the resultant due to the velocities v1{v_1} and v2{v_2}
θ\theta is the angle between the velocities v1{v_1} and v2{v_2}.
Equation 1 can be rewritten as,
Vr=3v3\Rightarrow {\vec V_r} = - 3{\vec v_3}
v3=13Vr\Rightarrow {\vec v_3} = - \dfrac{1}{3}{\vec V_r}
Let this be equation 2.
From equation 2, it is clearly evident that the velocity of the heavier particle will be one-third of the resultant velocity due to v1{v_1} and v2{v_2}. The negative sign indicates the direction of v3{v_3}is in the opposite direction of the resultant velocity.
v3=13Vr\Rightarrow {v_3} = - \dfrac{1}{3}{V_r}
v3=13×42.42=14.14ms1\Rightarrow {v_3} = \dfrac{1}{3} \times 42.42 = 14.14m{s^{ - 1}}
Therefore the velocity of the heavier particle will be 14.14ms114.14m{s^{ - 1}} in the opposite direction of the resultant of v1{v_1} and v2{v_2}.

Note: While solving these types of questions we should be very careful about the direction given in the question as momentum is a vector quantity. Also while using the conservation of momentum equation we should consider all the particles given in the system before and after an explosion or collision.