harsh95 said:
Sir,if it is given that mass of truck is greater then would it have a greater momenta?
What is the formula for momentum?
Also the collision lasts for 1 second,so how they have equal momenta?
What are their momenta after the collision and they are both at rest?
Could please tell me the answer for (c) and (d)
I am preparing for Science Olympiad and "Law of motion" is one of the chapter in syllabus.
Am really confused between 2nd and 3rd law!
How you answer (c) and (d) depends upon your understanding of the question. If you think that the truck has a different mass than the car, then they would have to have different velocities in order for the magnitudes of their momenta to be equal. With different momenta you would expect there to be some "leftover" momentum after the collision, and the pair would continue to roll or slide along the road until friction brought them to a halt.
Because 3rd law states that every action has equal and opposite reaction then but then F=ma.Then if the Mass of object and the acceleration is greater then the object it is having head on collision with then how will they exert equal force?
I think if understood this concept I would be able solve this type of question! Please help
Thank you
Suppose you have one mass M that is ten times another mass m. If mass M is traveling at speed V, what speed would m have to travel in order to have the same magnitude of momentum?
If both M and m are brought to rest by colliding head-on, what is the change in velocity of each? Which had to accelerate (decelerate) more during the collision?
The third law concerns bodies that mutually interact; One body touches another and they apply equal and oppositely directed forces on each other. The second law concerns an unbalanced external force being applied to a body, without reference to what the "agent" is that's applying the force.
In reality, all real forces have "agents" of some form if you look hard enough. But it is often convenient to ignore the agent and consider just the disembodied force. An example is the force of gravity, where we simply place a force vector on the free body diagram and label it "mg"; we (usually) don't bother considering the third-law implications of the response of the Earth to the equal and opposite force being applied to it.