Question #331229

momentum is conserved in a collision of two objects as measured by an observer on a uniformly moving train. show that momentum is also conserved for a ground observed



Expert's answer

Momentum conserving in the train reference system:

v1→+v2→=u1→+u2→,   (1)\overrightarrow{v_1}+\overrightarrow{v_2}=\overrightarrow{u_1}+\overrightarrow{u_2},~~~(1)

where v1→, v2→\overrightarrow{v_1},~\overrightarrow{v_2} - velocities of the first and second object before collision, u1→, u2→\overrightarrow{u_1},~\overrightarrow{u_2} - after collision.


In the ground reference system each of those velocities will be increased with velocity of train vv:

v1′→=v1→+v→⇒v1→=v1′→−v→,v2′→=v2→+v→⇒v2→=v2′→−v→,u1′→=u1→+v→⇒u1→=u1′→−v→,u2′→=u2→+v→⇒u2→=u2′→−v→\overrightarrow{v_1'}=\overrightarrow{v_1}+\overrightarrow{v}\Rarr \overrightarrow{v_1}=\overrightarrow{v_1'}-\overrightarrow{v},\\ \overrightarrow{v_2'}=\overrightarrow{v_2}+\overrightarrow{v}\Rarr \overrightarrow{v_2}=\overrightarrow{v_2'}-\overrightarrow{v},\\ \overrightarrow{u_1'}=\overrightarrow{u_1}+\overrightarrow{v}\Rarr \overrightarrow{u_1}=\overrightarrow{u_1'}-\overrightarrow{v},\\ \overrightarrow{u_2'}=\overrightarrow{u_2}+\overrightarrow{v}\Rarr \overrightarrow{u_2}=\overrightarrow{u_2'}-\overrightarrow{v}

Let's insert this values into the equation (1):

(v1′→−v→)+(v2′→−v→)=(u1′→−v→)+(u2′→−v→)⇒⇒v1′→+v2′→=u1′→+u2′→,(\overrightarrow{v_1'}-\overrightarrow{v})+(\overrightarrow{v_2'}-\overrightarrow{v})=(\overrightarrow{u_1'}-\overrightarrow{v})+(\overrightarrow{u_2'}-\overrightarrow{v})\Rarr\\ \Rarr\overrightarrow{v_1'}+\overrightarrow{v_2'}=\overrightarrow{u_1'}+\overrightarrow{u_2'},

so, we can see that momentum is also conserved in the ground reference system.


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