Conservation of momentum

Consider two interacting objects. If thing 1 pushes on thing 2 through a pressure F = 10 N because that 2 s come the right, then the momentum of object 2 alters by 20 Ns = 20 kgm/s come the right. By Newton"s third law thing 2 pushes on thing 1 with a pressure F = 10 N because that 2 s come the left. The inert of object 1 changes by 20 Ns = 20 kgm/s to the left. The total momentum that both objects does no change. Thus we say that the total momentum the the connecting objects is conserved.

Newton"s third law means that the total momentum of a device of communicating objectsnot acted on by exterior forces is conserved.

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The complete momentum in the universe is conserved. The momentum of a solitary object, however, alters when a net force acts on the object for a limited time interval. Vice versa, if no network force acts upon an object, its inert is constant.

For a mechanism of objects, a ingredient of the momentum along a liked direction is constant, if no net exterior force v a component in this preferred direction acts upon the system.


In collisions in between two diverted objects Newton"s third law means that momentum is constantly conserved. In collisions, it is assumed the the colliding objects interact for such a brief time, that the impulse due to external forces is negligible. Therefore the total momentum that the system just prior to the collision is the same as the full momentum simply after the collision. Collisions in i beg your pardon the kinetic energy is additionally conserved, which the kinetic energy just after ~ the collision amounts to the kinetic energy just prior to the collision, are dubbed elastic collision. In these collisions no ordered energy is converted into thermal energy. Collisions in which the kinetic energy is not conserved, i.e. In which part ordered energy is converted into internal energy, are dubbed inelastic collisions. If the two objects stick together after the collision and also move with a usual velocityvf, climate the collision is said to beperfectly inelastic.

Note:In collisions in between two secluded objects inert is always conserved.Kinetic power is just conserved in elastic collisions.

We always have m1v1i + m2v2i= m1v1f + m2v2f.Only because that elastic collisions do we also have ½m1v1i2+ ½m2v2i2 = ½m1v1f2+ ½m2v2f2.


If 2 objects collide and also one is initially at rest, is it possible for both to it is in at rest after the collision? Is it feasible for one to be at rest after the collision? Explain!


Reasoning:In collisions between two objects inert is conserved. Because the initial momentum is no zero, the final momentum is no zero. Both objects cannot be in ~ rest.It is possible for one of the objects to it is in at rest after the collision. Because that example, if the masses of the 2 objects are equal, then after a head-on elastic collision the object originally at rest is moving and the object initially moving is at rest.Problem:

A 10 g cartridge is stopped in a block of lumber (m = 5 kg). The rate of the bullet-wood mix immediately after the collision is 0.6 m/s. What was the original speed the the bullet?


Reasoning:This is a perfectly inelastic collision. The two objects stick together after the collision and move through a usual velocity v
f. I think the movement is follow me the x-direction. Us then havem1v1 + m2v2 = (m1 + m2)vf.m1 is the mass of the bullet, v1 its early velocity, m2 is the mass of the block, v2 its early velocity.Details that the calculation:Initially the block is at rest, v2 = 0. Therefore(0.01 kg)v1 = (5.01 kg)(0.6 m/s). V1 = 300.6 m/s.Problem:

Two dare of equal mass and equal speeds collide head on. Execute they endure a greater pressure if the collision is elastic or perfectly inelastic and they stick together?


Reasoning:Let the cars relocate along the z-axis. Once the collision is elastic, the readjust in inert of the auto moving originally in the positive x-direction is pfinal - pinitial = -2 pinitial, due to the fact that the car bounces ago and pfinal = -pinitial. When the collision is inelastic, the cars pertained to rest and also the change in inert of the automobile moving originally in the hopeful x-direction is pfinal - pinitial = pinitial, because pfinal = 0. For this reason the impulse has actually twice the size in the elastic collision. If the collisions last around the same amount the time, then the average force experienced by the vehicle is double as huge in the elastic collision.Problem:

A 90 kg fullback running east with a rate of 5 m/s is tackled through a 95 kg foe running north through a rate of 3 m/s. If the collision is perfect inelastic, calculation the speed and the direction of the players just after the tackle.


Reasoning:Momentum is a vector. In the collision, the complete momentum is conserved.Details the the calculation:The initial inert of player 1 is p
1 =(90 kg)(5 m/)s i = 450 kgm/s i.The initial inert of player 2 is p2 =(95 kg)(3m/s)j = 285 kgm/s j.Momentum is conserved, the last momentum p of both football player is p= p1 + p2.p = (m1 + m2)v.v = 2.432 m/si + 1.54 m/s j.v2 = 8.29 (m/s)2, v = 2.88 m/s.The rate of the football player after the collision is 2.88 m/s.tanθ = py/px = 285/450 = 0.63, θ = 32.34o.Their direction the travel provides an edge θ = 32.34o v the x-axis. (The x-axis is pointing east.)Problem:

A 30,000 kg freight vehicle is coasting in ~ 0.850 m/s v negligible friction under a hopper the dumps 110,000 kg of scrap metal into it. What is the last velocity the the loaded freight car?


Reasoning:For a system of objects, a ingredient of the momentum follow me a favored direction is constant, if no net exterior force v a component in this chosen direction acts on the system.Details of the calculation:Let the direction of motion of the vehicle be the optimistic x-direction.Before the intake the momentum of the auto was in the x-direction with magnitude p = mv = 2.55*104 kgm/s.The x- ingredient of the inert of the scrap steel was zero, so the total initial inert in the x-direction was pi = 2.55*104 kgm/s.No exterior force acts on the objects in the x-direction, thus the x-component the the complete momentum is = (mcar + mmetal)vf = (140,000 kg)vf = pi = 2.55*104 kgm/s.vf = (2.55*104 kgm/s)/(140,000 kg)= 0.182 m/s.Problem:

After a completely inelastic collision in between two objects of same mass, each having initial rate v, the two relocate off in addition to speed v/3. What was the angle between their initial directions?


Reasoning:The outside force acting on the system is zero, the full momentum is conserved.Assume the the last velocity the the objects points in the +x-direction. Prior to the collision the velocity vector of both objects provides an angle θ v the x-axis as shown.
Details the the calculation:p1x + p2x = pfx = pf, p1y+ p2y = 0.2mv cosθ = 2mv/3, cosθ = 1/3, θ = 70.5o.The angle between their initial directions is 2θ = 141o.Problem:

The fixed of the blue puck is 20% greater than the mass of the eco-friendly one. Before colliding, the pucks technique each various other with equal and opposite momenta, and also the eco-friendly puck has actually an initial rate of 10 m/s. Find the speed of the pucks ~ the collision, if fifty percent the kinetic power is lost during the collision.



Reasoning:The collision is inelastic, due to the fact that energy is not conserved.The complete momentum the the 2 pucks is zero prior to the collision and after the collision.Let fragment 1 be the environment-friendly puck and particle 2 it is in the blue puck. Before and after the collision the proportion of the speeds is v2/v1= m1/m2 = 1/1.2.The final kinetic energy of the system amounts to ½ time its initial kinetic energy.½m1v1i2+ ½m2v2i2 = 2*(½m1v1f2+ ½m2v2f2).Details that the calculation:½m1v1i2+ ½m2v2i2 = 2*(½m1v1f2+ ½m2v2f2).Algebra:m1v1i2+ m2v2i2 = 2 (m1v1f2 + m2v2f2).m1v1i2 + 1.2 m1(v1i/1.2)2= 2 (m1v1f2 + 1.2 m1(v1f/1.2)2).m1(v1i2 + v1i2/1.2) = 2 m1(v1f2 + v1f2/1.2).v1i2 = 2 v1f2, v1f = 0.707 v1i.v1f = 7.07 m/s, v2f = 5.89 m/s.Module 5: inquiry 1

During a visit come the International an are Station, one astronaut was positioned motionless in the center of the station, out of reach of any type of solid object on which he can exert a force. Indicate a an approach by i m sorry he might move himself away native this position, and also explain the chathamtownfc.netics involved.

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Module 5: concern 2

Football coaches advise players to block, hit, and also tackle through their feet ~ above the ground fairly than by leaping with the air. Making use of the ideas of momentum, work, and energy, describe how a football player have the right to be more effective through his feet ~ above the ground.