physics 207: lecture 8, pg 1 lecture 9 l goals describe friction in air (ch. 6) differentiate...
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Physics 207: Lecture 8, Pg 1
Lecture 9
GoalsGoals
Describe Friction in Air (Ch. 6)
Differentiate between Newton’s 1st, 2nd and 3rd Laws
Use Newton’s 3rd Law in problem solving
Assignment: HW4, (Chap. 6 & 7, due 10/5)
1st Exam Thurs., Oct. 7th from 7:15-8:45 PM Chapters 1-7
in rooms 2103, 2141, & 2223 Chamberlin Hall
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Physics 207: Lecture 8, Pg 2
Friction in a viscous mediumDrag Force Quantified
With a cross sectional area, A (in m2), coefficient of drag of 1.0 (most objects), sea-level density of air, and velocity, v (m/s), the drag force is:
D = ½ C A v2 c A v2 in Newtons
c = ¼ kg/m3
In falling, when D = mg, then at terminal velocity Example: Bicycling at 10 m/s (22 m.p.h.), with projected
area of 0.5 m2 exerts a force of ~30 Newtons At low speeds air drag is proportional to v but at high
speeds it is v2
Minimizing drag is often important
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Physics 207: Lecture 8, Pg 3
Newton’s Third Law:
If object 1 exerts a force on object 2 (F2,1 ) then object 2
exerts an equal and opposite force on object 1 (F1,2)
F1,2 = -F2,1
IMPORTANT: Newton’s 3rd law concerns force pairs whichact on two different objects (not on the same object) !
For every “action” there is an equal and opposite “reaction”
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Physics 207: Lecture 8, Pg 4
Force Pairs vs. Free Body Diagrams
Consider the following two cases (a falling ball and ball on table),
Compare and contrast Free Body Diagram and
Action-Reaction Force Pair sketch
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Physics 207: Lecture 8, Pg 5
Free body diagrams
mg
mg
FB,T= N
Ball FallsFor Static Situation
N = mg
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Physics 207: Lecture 8, Pg 6
Force Pairs
1st and 2nd Laws Free-body diagram Relates force to acceleration3rd Law Action/reaction pairsShows how forces act between objects
FB,E = -mg FB,T= N
FE,B = mg
FB,E = -mg
FE,B = mg
FT,B= -N
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Physics 207: Lecture 8, Pg 7
Example (non-contact)
Consider the forces on an object undergoing projectile motion
FB,E = - mB g
EARTH
FE,B = mB g
FB,E = - mB g
FE,B = mB g
Question: By how much does g change at an altitude of 40 miles? (Radius of the Earth ~4000 mi)
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Physics 207: Lecture 8, Pg 8
Note on Gravitational Forces
Newton also recognized that gravity is an attractive, long-range force between any two objects.
When two objects with masses m1 and m2 are separated by distance r, each object “pulls” on the other with a force given by Newton’s law of gravity, as follows:
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Physics 207: Lecture 8, Pg 9
Cavendish’s Experiment
F = m1 g = G m1 m2 / r2
g = G m2 / r2
If we know big G, little g and r then will can find m2 the mass of the Earth!!!
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Physics 207: Lecture 8, Pg 10
Example (non-contact)
Consider the force on a satellite undergoing projectile motion 40 km above the surface of the earth:
FB,E = - mB g
EARTH
FE,B = mB g
FB,E = - mB g
FE,B = mB g
Compare: g = G m2 / 40002 g’ = G m2 / (4000+40)2
g / g’ = / (4000+40)2 / 40002 = 0.98
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Physics 207: Lecture 8, Pg 11
A conceptual question: A flying bird in a cage
You have a bird in a cage that is resting on your upward turned palm. The cage is completely sealed to the outside (at least while we run the experiment!). The bird is initially sitting at rest on the perch. It decides it needs a bit of exercise and starts to fly.
Question: How does the weight of the cage plus bird vary when the bird is flying up, when the bird is flying sideways, when the bird is flying down?
Follow up question:
So, what is holding the airplane up in the sky?
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Physics 207: Lecture 8, Pg 12
Static Friction with a bicycle wheel
You are pedaling hard and the bicycle is speeding up.
What is the direction of the frictional force?
You are breaking and the bicycle is slowing down
What is the direction of the frictional force?
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Physics 207: Lecture 8, Pg 13
Exercise Newton’s Third Law
A. greater than
B. equal to
C. less than
A fly is deformed by hitting the windshield of a speeding bus.
v
The force exerted by the bus on the fly is,
that exerted by the fly on the bus.
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Physics 207: Lecture 8, Pg 14
Exercise 2Newton’s Third Law
A. greater than
B. equal to
C. less than
A fly is deformed by hitting the windshield of a speeding bus.
v
The magnitude of the acceleration, due to this collision, of the bus is
that of the fly.
Same scenario but now we examine the accelerations
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Physics 207: Lecture 8, Pg 15
Exercise 3Newton’s 3rd Law
A. 2
B. 4
C. 6
D. Something else
a b
Two blocks are being pushed by a finger on a horizontal frictionless floor.
How many action-reaction force pairs are present in this exercise?
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Physics 207: Lecture 8, Pg 16
Force pairs on an Inclined plane
Forces on the block
Block weight is mg
NormalForce
Friction Force
“Normal” means perpendicular
mg cos
f
x
y
mg sin
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Physics 207: Lecture 8, Pg 17
Force pairs on an Inclined plane
Forces on the block (equilibrium case)
NormalForce
Friction Force
f= N
x
yForces on the plane
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Physics 207: Lecture 8, Pg 18
Force pairs on an Inclined plane
Forces on the block (non equilibrium case)
NormalForce
Friction Force
f
x
yForces on the plane
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Physics 207: Lecture 8, Pg 19
Example: Friction and Motion
A box of mass m1 = 1 kg is being pulled by a horizontal string having tension T = 40 N. It slides with friction
(k= 0.5) on top of a second box having mass m2 = 2 kg, which in turn slides on a smooth (frictionless) surface. What is the acceleration of the second box ?
1st Question: What is the force on mass 2 from mass 1?
(A) a = 0 N (B) a = 5 N (C) a = 20 N (D) can’t tell
mm22
T mm11slides with friction (k=0.5)
slides without frictiona = ?
v
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Physics 207: Lecture 8, Pg 20
ExampleSolution
First draw FBD of the top box:
m1
N1
m1g
T fk = KN1 = Km1g
v
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Physics 207: Lecture 8, Pg 21
Newtons 3rd law says the force box 2 exerts on box 1 is equal and opposite to the force box 1 exerts on box 2.
m1ff1,2 = Km1g = 5 N
m2
ff2,1 == -ff1,2
As we just saw, this force is due to friction:
ExampleSolution
ActionReaction
(A) a = 0 N (B) a = 5 N (C) a = 20 N (D) can’t tell
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Physics 207: Lecture 8, Pg 22
Now consider the FBD of box 2:
m2 ff2,1 = km1g
m2g
N2
m1g
ExampleSolution
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Physics 207: Lecture 8, Pg 23
Finally, solve Fx = ma in the horizontal direction:
m2 ff2,1 = Km1g
K m1g = m2a
ExampleSolution
= 2.5 m/s2
kg 2
N 5ga
2
k1
m
m
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Physics 207: Lecture 8, Pg 24
Home Exercise Friction and Motion, Replay
A box of mass m1 = 1 kg, initially at rest, is now pulled by a horizontal string having tension T = 10 N. This box (1) is on top of a second box of mass m2 = 2 kg. The static and kinetic coefficients of friction between the 2 boxes are s=1.5 and k= 0.5. The second box can slide freely (frictionless) on an smooth surface.
Compare the acceleration of box 1 to the acceleration of box 2 ?
mm22
T mm11
friction coefficients s=1.5 and k=0.5
slides without frictiona2
a1
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Physics 207: Lecture 8, Pg 25
Home Exercise Friction and Motion, Replay in the static case
A box of mass m1 = 1 kg, initially at rest, is now pulled by a horizontal string having tension T = 10 N. This box (1) is on top of a second box of mass m2 = 2 kg. The static and kinetic coefficients of friction between the 2 boxes are s=1.5 and k= 0.5. The second box can slide freely on an smooth surface (frictionless).
If no slippage then the maximum frictional force between 1 & 2 is
(A) 20 N (B) 15 N (C) 5 N (D) depends on T
mm22
T mm11friction coefficients
s=1.5 and k=0.5
slides without frictiona2
a1
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Physics 207: Lecture 8, Pg 26
Home ExerciseFriction and Motion
fs = 10 N and the acceleration of box 1 is
Acceleration of box 2 equals that of box 1, with |a| = |T| / (m1+m2) and the frictional force f is m2a
(Notice that if T were in excess of 15 N then it would break free)
mm2 2
T mm11
friction coefficients s=1.5 and k=0.5
slides without frictiona2
a1
TTm1 gg
NN
fS
fS S N = S m1 g = 1.5 x 1 kg x 10 m/s2
which is 15 N (so m2 can’t break free)
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Physics 207: Lecture 8, Pg 27
Recap
Wednesday: Review for exam