msu physics 231 fall 2015 1 physics 231 topic 6: momentum and collisions alex brown october 7 2015
TRANSCRIPT
MSU Physics 231 Fall 2015 1
Physics 231Topic 6: Momentum and Collisions
Alex BrownOctober 7 2015
MSU Physics 231 Fall 2015 2
MSU Physics 231 Fall 2015 3
MomentumF = m a Newton’s 2nd lawF = m v/t a=v/tF = m (vfinal - vinital)/t
Define p = mv momentum (kg m/s)
F= (pfinal - pinitial)/tF= p/t = m v/t p = (pfinal - pinitial) = m v impulse
The net force acting on an object equalsthe change in momentum (p) in time period (t). Since velocity is a vector, momentum is alsoa vector, pointing in the same direction as v.
MSU Physics 231 Fall 2015 4
ImpulseF=p/t Force=change in (mv) per time
period (t).p=Ft The change in momentum equals
the force acting on the object timeshow long you apply the force.
Definition: p = Impulse
What if the force is not constant within the timeperiod t?
ts s s
F1
F2
F3
p = (F1 t + F2 t + F3 t)
= area under F vs t plot
MSU Physics 231 Fall 2015 5
car hitting haystack and stoping
car hitting wallThe change in momentum (impulse) is the same, but the forcereaches a much higher value when the car hits a wall!
MSU Physics 231 Fall 2015 6
Some examplesA tennis player receives a shot approaching him (horizontally) with 50m/s and returns the ball in the opposite direction with 40m/s. The mass of the ball is 0.060 kg.A) What is the impulse delivered by the ball to the racket?B) What is the change in kinetic energy of the ball?
A) Impulse=change in momentum (p). p = m (vfinal - vinitial) = 0.060(-40-50) = -5.4 kg m/s
B) KEi = 75 J KEf = 48 J (no PE!) Enc = KEi - KEf = 27 J (energy lost to heat)
MSU Physics 231 Fall 2015 7
Child safetyA friend claims that it is safe to go on a car trip with yourchild without a child seat since he can hold onto your 12kg child even if the car makes a frontal collision (lasting 0.05s and causing the vehicle to stop completely) at v=50 km/h(about 30 miles/h). Is he to be trusted?
F = p/t force = impulse per time period = m (vf-vi) /t vf = 0 and vi = 50 km/h = 13.9 m/s m = 12kg t=0.05s
F = 12(-13.9)/0.05 = -3336 N
This force corresponds to lifting a mass of 340 kg!!!
MSU Physics 231 Fall 2015 8
Question (assume t is the same for both cases)
The velocity change is largest in case: A B
The acceleration is largest in case: A B
The momentum change is largest in case: A B
The impulse is largest in case: A B
MSU Physics 231 Fall 2015 9
F21 t = p1 = p1f - p1i
F12 t = p2 = p2f – p2i
Newton’s 3rd law: F12 = - F21
F12 t = - F21 t
p1f - p1i = - p2f + p2i
Rewrite: p1i + p2i = p1f + p2f
CONSERVATION OF MOMENTUM(only for a closed system)
Conservation of Momentum
m1m2
p1i p2i
m1m2
Force of 2 on 1 = F21 F12
m1
p1f m2
p2f
p1 = m1 v1
p2 = m2 v2
MSU Physics 231 Fall 2015 10
questionAn object is initially at rest in outer space (no gravity).It explodes and breaks into two pieces, not of equal size.The magnitude of the momentum of the larger piece is …a) Greater than that of the smaller pieceb) Smaller than that of the smaller piecec) The same as that of the smaller piece
Initial momentum is zero0 = plarge,final + psmall,final
So plarge,final = - psmall,final
Magnitude is the same, direction opposite.
MSU Physics 231 Fall 2015 11
QuizAn object is initially at rest in outer space (no gravity).It explodes and breaks into three pieces, not of equal size.The momentum of the largest piece:a) Must be larger than that of each of the smaller piecesb) Must be less than that of each of the smaller piecesc) Must be equal in magnitude but opposite in direction to the
sum of the smaller pieces.d) Cannot be determined from the momenta of the smaller
piecesThe conservation of momentum must hold, even with more than 2 objects. Although the momenta of each piece could be pointing in a different direction, the sum must be equal to zero after the explosion. So, the momentum of one of the pieces must always be opposite in direction, but equal in magnitude to the sum of the momenta of the other two pieces.
MSU Physics 231 Fall 2015 12
Moving in spaceAn astronaut (100 kg) is drifting away from the spaceship with v=0.2 m/s. To getback he throws a wrench (2 kg) in the direction away from the ship. With whatvelocity does he need to throw the wrenchto move with v=0.1 m/s towards the ship?
Initial momentum: mavai + mwvwi =100*0.2+2*0.2 = 20.4 kg m/sAfter throw: mavaf + mwvwf = 100*(-0.1) + 2*vwf kg m/s
Conservation of momentum: mavai + mwvwi = mavaf + mwvwf
20.4 = -10 + 2*vwf vwf=15.7 m/s
(a) 0.1 m/s (b) 0.2 m/s (c) 5 m/s (d) 16 m/s(e) this will never work?
MSU Physics 231 Fall 2015 13
Perfectly inelastic collisions Conservation of momentum: m1v1i+m2v2i=m1v1f+m2v2f
After the collision m1 and m2 form one new object with massM = m1 + m2 and one velocity vf =v1f = v2f
m1v1i + m2v2i = vf (m1 + m2)
vf = (m1v1i + m2v2i)/ (m1 + m2)
before after
Demo: perfect inelastic collision on airtrack
MSU Physics 231 Fall 2015 14
Perfectly inelastic collisions Conservation of momentum: m1v1i+m2v2i=m1v1f+m2v2f
After the collision m1 and m2 form one new object with massM = m1 + m2 and one velocity vf =v1f = v2f
m1v1i + m2v2i = vf (m1 + m2)vf = (m1v1i + m2v2i)/ (m1 + m2)
Let c = m2/m1 then
vf = (v1i + c v2i)/ (1+c)
If m1 = m2 (c=1) then vf = (v1i + v2i)/ 2
If c=1 and v2i = 0 then vf = v1i/2
MSU Physics 231 Fall 2015 15
Perfect inelastic collision: an example
A car collides into the back of a truck and their bumpers getstuck. What is the ratio of the mass of the truck and the car?(mtruck/mcar = m2/m1 =c) What is the fraction of KE lost?
50 m/s 20 m/s 25 m/s
Before collision: KEi = ½m1(50)2 + ½5m1(20)2
After collision: KEf = ½6m1(25)2
Ratio: KEf/KEi= [6*(25)2]/[(50)2+5*(20)2] = 0.8317% of the KE is lost (damage to cars!)
vf = [v1i + cv2i] / (1+c) solve for c
c = [v1i - vf] / [vf – v2i] = (50-25)/(25-20) = 5
MSU Physics 231 Fall 2015 16
Types of collisionsInelastic collisions Elastic collisions
•Momentum is conserved
•Some energy is lost in the collision: kinetic energy is not conserved
•Perfectly inelastic: the objects stick together.
•Momentum is conserved
•No energy is lost in the collision: kinetic energy is conserved
KEi - KEf = Enc KEi - KEf = 0
MSU Physics 231 Fall 2015 17
Inelastic Solution
vf = [m1 v1i + m2v2i] / (m1+m2)
With m2 = c m1
vf = [v1i + cv2i] / (1+c)
Special case m2 = m1 (c=1)
vf = [v1i + v2i] / 2
Conservation of momentum: m1v1i + m2v2i = m1v1f + m2v2f
After the collision m1 and m2 form one new object with massM = m1 + m2 and one velocity vf =v1f = v2f
m1v1i + m2v2i = vf (m1 + m2)KEi - KEf = Enc
MSU Physics 231 Fall 2015 18
Elastic collisionsConservation of momentum: m1v1i+m2v2i=m1v1f+m2v2f
Conservation of KE: ½m1v1i
2+½m2v2i2=½m1v1f
2+½m2v2f2
Two equations and two unknowns – after some algebra (see book)
MSU Physics 231 Fall 2015 19
Elastic Solution
v1f = [(m1 –m2) v1i + 2m2v2i] / (m1+m2)
v2f = [(m2 –m1) v2i + 2m1v1i] / (m1+m2)
For m2 = c m1
v1f = [(1-c) v1i + 2cv2i] / (1+c)
v2f = [(c-1) v2i + 2v1i] / (1+c)
Special case m2 = m1 (c=1)
v1f = v2i
v2f = v1i
KEi - KEf = 0
MSU Physics 231 Fall 2015 20
Given m2=m1 and v1i=0
What are the velocities of m1 and m2 after the collision in terms of the initial velocity of m2 if m1 is originally at rest?
c = 1v1f = v2i
v2f = v1i = 0
m1 m2
m1 m2
Elastic collisions of equal mass
For m2 = c m1
v1f = [(1-c) v1i + 2cv2i] / (1+c)
v2f = [(c-1) v2i + 2v1i] / (1+c)
MSU Physics 231 Fall 2015 21
Collisions in one dimension given
given m1 and m2 or c = m2 /m1
v1i and v2i
Elastic (KE conserved)
v1f = [(1-c) v1i + 2c v2i] / (1+c)
v2f = [(c-1) v2i + 2v1i] / (1+c)
Inelastic (stick together, KE lost)
vf = [v1i + c v2i] / (1+c)
Momentum p = mvImpulse p = pf - pi = FtConservation of momentum (closed system) p1i + p2i = p1f + p2f
MSU Physics 231 Fall 2015 22
inelastic collision
With m2 = c m1
vf = [v1i + cv2i] / (1+c)
MSU Physics 231 Fall 2015 23
elastic collisions
For m2 = c m1
v1f = [(1-c) v1i + 2cv2i] / (1+c)
v2f = [(c-1) v2i + 2v1i] / (1+c)
MSU Physics 231 Fall 2015 24
elastic collisions
For m2 = c m1
v1f = [(1-c) v1i + 2cv2i] / (1+c)
v2f = [(c-1) v2i + 2v1i] / (1+c)
MSU Physics 231 Fall 2015 25
Clicker Quiz
In a system with 2 moving objects when a collision occursbetween the objects:a) the total kinetic energy is always conservedb) the total momentum is always conservedc) the total kinetic energy and total momentum are always conservedd) neither the kinetic energy nor the momentum is conserved
For both inelastic and elastic collisions, the momentum isconserved.
MSU Physics 231 Fall 2015 26
Clicker QuizBA
Consider a closed system of objects A and B.Object A is thrown at an object B that was originally at rest, as shown
in the figure. It is not known if A is heavier or lighter than B. After A collides with B:
a) Object A must go left (back in the direction it came from)b) Object A must go rightc) Object A could go left or rightd) Object B could go lefte) The total momentum will be different than before the collision
If the collision is perfectly inelastic. A & B stick together and must go right (conservation of momentum). If the collision is elastic and mA<<mB A will go left. If mA>>mB both will go right. So A could go left or right. B can not go left (A would have to go left to, which violates momentum conservation.
MSU Physics 231 Fall 2015 27
Ballistic Pendulumblockm2=1 kgv2i = 0
bulletm1 = 0.1 kgvb = v1i = ? h=0.2m
What is the speed of the bullet?
There are 2 stages:• The collision• The swing up
The swing of the block Use conservation of Mechanical energy. (M g y + ½Mv2)bottom = (M g y + ½Mv2)top M = m1 +m2
0 + ½M(vf)2 = ½M(vb)2/(1+c)2 = Mgh gives (vb)2 = 2 g h (1+c)2
The collision The bullet gets stuck in the block (perfect inelastic collision). Use conservation of momentum.
c = (m2/m1) = 10 vf = (v1i + c v2i)/(1+c) = vb/(1+c)
vb = 21.8 m/s
MSU Physics 231 Fall 2015 28
Clicker Quiz
The kinetic energy of an object is quadrupled. Its momentum will change by a factor of…
a) 0b) 2c) 4d) 8e) 16
MSU Physics 231 Fall 2015 29
Impact of a meteoriteEstimate what happens if a 2.8x1013 kg meteorite collides with earth:
a) Is the orbit of earth around the sun changed?b) how much energy is released?Assume: meteorite has same density as earth, the collision isinelastic and the meteorite’s v is 10 km/s (relative to earth)
A) Earth’s mass: me = 6x1024kg mm = 2.8x1013 kg ve=0 vm=1x104 m/s
Conservation of momentum: c = me/mm= 2.14 x 1011
vf = vm /(1+c) vf=4.7x10-8 m/s (very small)B) Energy=Kinetic energy loss: (½meve
2+½mmvm2) - (½mmevme
2)
0 + 0.5 (2.8x1013) (1x104)2 - 0.5 (6x1024) (4.7x10-8)2 = 1.4x1021 J
Largest nuclear bomb existing: 100 megaton TNT = 4.2x1017 JEnergy release: 3300 nuclear bombs!!!!!
MSU Physics 231 Fall 2015 30
problemm1=5 kg m2=10 kg. M1 slides down and makesan elastic collision with m2. How high doesm1 go back up?
ME = mgh + (1/2)mv2
Step 1. What is the velocity of m1 just before it hits m2?Conservation of ME: MEtop= MEbottom = m1gh + 0 = 0 + 0.5m1v2
So v1 = 9.9 m/s
Step 2. Elastic collision with c = 2, v1i = 9.9 and v2i = 0
so v1f = -3.3
Step 3. m1 moves back up; use conservation of ME again.MEtop= MEbottom = m1gh’ + 0 = 0 + 0.5 m1 v1f
2
So h’ = 0.55 m
h=5m
m1
m2
MSU Physics 231 Fall 2015 31
Playing with blocksm1=0.5 kg collision is elasticm2=1.0 kgh1=2.5 mh2=2.0 m
A) determine the velocity of the blocks after the collisionB) how far away from the bottom of the table does m2 land
MSU Physics 231 Fall 2015 32
Determine the velocity of the blocks after the collision
m1=0.5 kg collision is elasticm2=1.0 kgh1=2.5 mh2=2.0 m
Step 1: determine velocity of m1 at the bottom of the slideConservation of ME (mgh+½mv2)top =(mgh+½mv2)bottom
0.5*9.81*2.5 + 0 = 0 + 0.5*0.5*v2
so: v1=7.0 m/sStep 2: Elastic collision equation with c = 2, v1i = 7 and v2i = 0
Gives v1f = -2.33 and v2f = 4.67
MSU Physics 231 Fall 2015 33
How far away from the table does m2 land?
m1=0.5 kg collision is elasticm2=1.0 kgh1=2.5 mh2=2.0 mv1f=-2.3 m/s v2f=4.7 m/s
This is a parabolic motion with initial horizontal velocity.Horizontal vertical
x = vxot y = yo + vyot - ½gt2
x = 4.7 t 0 = 2.0 + 0 - 0.5*9.81*t2
= 2.96 m t=0.63 s
MSU Physics 231 Fall 2015 34
atvv yy 0
221 attvy oy
221 attvy y
tvvy yoy )(21
)( 20
2
21
yya vvy
(A)
(B)
(C)
(D)
(E)
with a = -g
MSU Physics 231 Fall 2015 35
at the top all have vy = 0 (why?) at the top and bottom vx (Q) < vx (N) (why?)at the top vx (P) = vx (R) = 0 (why?)For all (PE+KE) (bottom) = (PE+KE) (top) mvo
2/2 = m(vox2 + voy
2)/2 = mgh + [mvx2/2]
For Q and N get time from (Eq. C)
MSU Physics 231 Fall 2015 36
a) Speed at X compared to V ? b) Velocity at X compared to P ? c) Size of total force at R compared to T ? d) Size of total force at Q compared to T ?
MSU Physics 231 Fall 2015 37
a) Speed at X compared to V ? X larger than Vb) Velocity at X compared to P ? samec) Size of total force at R compared to T ? T larger than Rd) Size of total force at Q compared to T ? Q larger than T
MSU Physics 231 Fall 2015 38
Remember at the a given time Power = P = F v = m a v
MSU Physics 231 Fall 2015 39
questionA girl (g) is standing on a plank (p) that is lying on ice (assume frictionless surface between ice and board). She starts to walk with 1 m/s, relative to the plank. What is her speed relative to the ice? Use mg=70 kg mp=100 kgChoose the ice as a frame of referenceInitial: both she and the plank are at rest.Final: vgp = vg – vp =1 vgp = velocity of girl relative to plank vg = velocity of girl relative to icevp = vg - vgp vp = velocity of plank relative to ice
Conservation of momentum: Initial (not moving): =0Final: mg vg+ mp vp = mg vg + mp(vg-vgp) = 70 vg + 100(vg-1) = 0
Solve for vg = 0.59 m/s