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the product of mass and velocity, a vector quantity known as (blank) and denoted by p
linear momentum
p = mv
A large force that acts for a short period of time can produce the same change in linear momentum as a (blank) acting for a greater period of time
small force
The equation if we take the average force that acts over the time interval t
F = p/t
F = p/t becomes F= ma since (blank)
p/1 = mv/t = m (v/t) = ma
The product of force and the time during which it acts is known as (blank) it’s a vector quantity that’s denoted by J
impluse
J = Ft
Impulse is equal to change in linear momentum. In terms of impulse, Newton’s second law can be written in yet another form
J = p
The impulse delivered to an object may be found by taking the area under a (blank) graph
force-versus time
The impulse-momentum theorem states than an impulse that is delivered on an (blank) Therefore the momentum after the collision is equal to the (blank)
object changes to momentum
momentum before
Pfinal = Pinitial + J
The total linear momentum of an isolated system remains (blank)
constant
Law of conservation of momentum which states:
totalPinitial = totalPfinal
although the objects exert forces on each other during the impact, these forces are only (blank) and the system’s total linear momentum is conserved
internal
Elastic Collision
The objects bounce perfectly off each other in opposite directions
Kinetic energy is conserved. Momentum is conserved
m1v1 + m2v2 = m1v3 + m2m4
Inelastic Collision
The objects travel in the same direction after the collision
Kinetic energy is lost. Momentum is conserved
m1v1 + m2v2 = m1v3 + m2m4
Perfectly Inelastic Collision
The objects stick together and travel in the same direction
Greatest kinetic energy is lost. Momentum is conserved.
m1v1 + m2v2 = (m1 +m2)v3