Chapter 6: Momentum and Collisions. Section 6 – 1 Momentum and Impulse.
Monday, October 5, 1998 Chapter 5: Springs Chapter 6: Linear Momentum Conservation of Momentum...
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Transcript of Monday, October 5, 1998 Chapter 5: Springs Chapter 6: Linear Momentum Conservation of Momentum...
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Monday, October 5, 1998
Chapter 5: SpringsChapter 6: Linear Momentum
Conservation of Momentum Impulse
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A 600 kg elevator startsfrom rest and is pulledupward by a motor witha constant accelerationof 2 m/s2 for 3 seconds.What is the averagepower output of the motorduring this time period?
Fnet = ma = (600 kg)(2 m/s2)
Fnet = 1200 N = Fmotor - Fg = Fmotor - mg
1200 N = Fmotor - (600 kg)(10 m/s2) = Fmotor - 6000 N
Fmotor = 6000 N + 1200 N = 7200 N
Let’s first figure out theforce delivered by themotor...
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A 600 kg elevator startsfrom rest and is pulledupward by a motor witha constant accelerationof 2 m/s2 for 3 seconds.What is the averagepower output of the motorduring this time period?
Now we need todetermine the workdone by the motor...
W = F s But we don’t know s, so….
s = s0 +v0t +0.5at2 = 0 + 0 + 0.5(2 m/s2)(3 s)2 = 9 m
W = (7200 N)(9 m) = 64800 J
PW
t
64800
321600
J
s W
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In addition to the gravity, there are othermechanisms to store POTENTIAL ENERGY.One of them is...
Sir Robert Hooke unlocked the secretof the spring...
A spring resting in its natural state, with alength l exerts no horizontal force on anything!
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However, if we compress or stretch the springby some amount x, then the spring is observedto exert a Force in the opposite direction.
Hook discovered this force could be modeledby the mathematical expression
F = - kxNotice that this force operates along a linear line!
l x
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Which means that if we looked at the plotof Force versus compression/stretching x...
For
cex
Slope of this lineis -k, where k isthe spring constant.
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For
ce
x
If we look at the work done by an appliedforce which compresses the spring througha distance (-x1)...
-x1
F1
W F s Fx F x 11
2 1 0( )
W k x x kx 1
2 1 11
22( )( )
Work done BY theexternal force ONthe spring.
This energy is stored in the spring...
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PE kxspring 1
22Potential Energy of a spring is
So, for spring problems, we have a newTOTAL MECHANICAL ENERGY given by
KE PE PEg spring
And it is THIS quantity which will be conservedabsent other, outside forces.
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Momentum & Collisions
The linear momentum of an object of mass mmoving with velocity v is defined as theproduct of the mass and the velocity:
p mv
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p mv
Notice that momentum is a vector quantity,which means that it must be specified withboth a magnitude and direction.
Also notice that the direction of themomentum vector is necessarily parallelto the velocity vector.
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p mv
[ ] [ ][ ] p m v
[ ]p kg (m / s)
[ ]p N s
OR The units suggesta relationship betweenforce and momentum.
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p mv
What happens when we apply a forceto an object?
It accelerates.
Its velocity changes.
The force imparts momentum.
Its momentum changes.
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p mv
By how much will the momentum change?
That depends upon the length of time overwhich the force is applied to the object.
v v a t 0
mv mv ma t 0
mv mv F t 0
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mv mv F t 0
p p F t 0
p F t I Impulse
Change inmomentum
The impulse of a force on an object equals thechange in momentum of that object.
Notice that impulse is a vector quantity as well!