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Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics. Here's our statement of the conservation of linear momentum: Topic 2.2 Extended C – Conservation of linear momentum The total linear momentum of a system is conserved if the net external force acting on the system is zero. FYI: Another type of momentum is angular momentum. This type of momentum is not considered in this chapter. In mathematical symbols we have If F ext = 0 then P = 0 P 0 = P f Conservation of Linear Momentum FYI: We use a capital P to represent the total momentum of a system of more than one particle. Lower case p is used for single particles.

Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics. Here's our statement of the conservation

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Page 1: Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.  Here's our statement of the conservation

Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.

Here's our statement of the conservation of linear momentum:

Topic 2.2 ExtendedC – Conservation of linear momentum

The total linear momentum of a system is conserved if the net external force acting on the system is zero.

FYI: Another type of momentum is angular momentum. This type of momentum is not considered in this chapter.

In mathematical symbols we have

If Fext = 0 thenP = 0P0 = Pf

Conservation of Linear Momentum

FYI: We use a capital P to represent the total momentum of a system of more than one particle. Lower case p is used for single particles.

Page 2: Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.  Here's our statement of the conservation

PROOF OF THE CONSERVATION OF LINEAR MOMENTUMRecall Newton's 2nd law (p-form):

Topic 2.2 ExtendedC – Conservation of linear momentum

Fnet =pt

Newton's Second Law (p-form)

We begin by dividing the net force into all of its individual forces - both external and internal:

Fnet = F1,ext +...+ Fn,ext + F1,int +...+ Fm,int

From Newton's 3rd law, every internal force has an equal and opposite reaction force. Therefore, the sum of the internal forces is zero.

FYI: In any system, the internal forces will sum to ZERO.

Now if the external forces also sum to zero, we have

Fnet = 0 so that 0 = p

t. Thus P = 0. //

Page 3: Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.  Here's our statement of the conservation

Topic 2.2 ExtendedC – Conservation of linear momentum

Here’s a sample problem:Suppose a .02-kg bullet traveling horizontally at 300 m/s strikes a 4-kg block of wood resting on a wood floor. (a) How fast is the block/bullet combo moving immediately after collision?

If we consider the bullet-block combo as our system, there are no external forces in the x-direction. Thus

Pf = Pi

mvf + MVf = mvi + MVi

.02v + 4v = (.02)(300) + 4(0)

4.02v = 6

v = 1.49 m/s

the bullet and the block move at the same speed after collision

Page 4: Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.  Here's our statement of the conservation

Topic 2.2 ExtendedC – Conservation of linear momentum

Here’s a sample problem:Suppose a .02-kg bullet traveling horizontally at 300 m/s strikes a 4-kg block of wood resting on a wood floor. (b) If the block/bullet combo slides 4 m before coming to a stop, what is the coefficient of kinetic friction between the block and the floor?

We can use conservation of energy to solve this problem:

∆K + ∆U = Wnc

4 m

K – K0 + ∆U = -fkd0 0

(m+M)v02 = μkNd

12(m+M)v0

2 = μk(m+M)gd12

μk =v0

2

2gd

μk =1.492

2(10)(4)

μk = 0.027

Page 5: Along with the conservation of energy, conservation of momentum makes the second of two pillars used in physics.  Here's our statement of the conservation

Topic 2.2 ExtendedC – Conservation of linear momentum

Here’s a sample problem:Suppose a .02-kg bullet traveling horizontally at 300 m/s strikes a 4-kg block of wood resting on a wood floor. (c) How much energy is lost during the collision?

The energy lost is kinetic:

∆K = K – K0

(m+M)vf2 – mvi

212

∆K = 12

(4.02)1.492 – (0.02)300212

∆K = 12

∆K = -895.53 J