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Physics 211: Lecture 7 Todays Agenda

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Title: Physics 211: Lecture 7 Todays Agenda


1
Physics 211 Lecture 7Todays Agenda
  • Friction
  • What is it?
  • How do we characterize it?
  • Model of friction
  • Static Kinetic friction (kinetic dynamic in
    some languages)
  • Some problems involving friction

2
Trivia
  • At the surface of the earth, a gas occupies about
    1000 times as much volume as the same number of
    atoms in the liquid state.
  • On average, about how much further apart are the
    atoms in a gas than those in a liquid??
  • A factor of 10
  • A factor of 100
  • A factor of 1,000
  • A factor of 10,000

3
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5
New Topic Friction
  • What does it do?
  • It opposes relative motion of two objects that
    touch!

j
N
FAPPLIED
i
ma
some roughness here
mg
6
Surface Friction...
  • Friction is caused by the microscopic
    interactions between the two surfaces

Friction causes heat !
7
Atomic force microscope
  • Very fine tip scans over surface
  • Scan resolution atomic size!

http//stm2.nrl.navy.mil/how-afm/how-afm.html http
//en.wikipedia.org/wiki/Atomic_force_microscope
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10
Surface Friction...
  • Force of friction acts to oppose relative motion
  • Parallel to surface.
  • Perpendicular to Normal force.

j
N
F
i
ma
fF
mg
11
Model for Sliding (kinetic) Friction
  • The direction of the frictional force vector is
    perpendicular to the normal force vector N in the
    direction that opposes relative motion between
    the two surfaces.
  • The magnitude of the frictional force vector fF
    is proportional to the magnitude of the normal
    force N .
  • fF ?K N ( ?K??mg in the previous
    example)
  • The heavier something is, the greater the
    friction will be...makes sense!
  • The constant ?K is called the coefficient of
    kinetic friction.

12
Model...
  • Dynamics
  • i F ? ?KN ma
  • j N mg
  • so F ???Kmg ma

j
N
F
i
ma
?K mg
mg
13
Lecture 7, Act 0Friction
  • A small box of mass is being pulled to the right
    by a horizontal string. It slides with friction
    on top of a bigger box. Assume both boxes were
    initially at rest.
  • In which direction does the frictional force act
    on the bottom box?
  • A) To the right
  • B) To the left
  • C) Friction does not effect the bottom box, only
    the top box.

T
m

friction
M
14
Lecture 7, Act 0Solution
  • Draw FBD of the top box

N
T
f mKN mKmg
m
mg
15
Lecture 7, Act 0Solution
  • 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.

f1,2
m
f2,1
mKmg
M
16
Lecture 7, Act 1More Friction
  • A box of mass m 1.5 kg is being pulled by a
    horizontal string having tension T 90 N. It
    slides with friction (mk 0.51) on top of a
    second box having mass M 3 kg, which in turn
    slides on a frictionless floor.
  • What is the acceleration of the bottom box ?
  • (a) a 0 m/s2 (b) a 2.5 m/s2 (c) a 3.0
    m/s2

T
m


mk0.51
no friction
M
17
Lecture 7, Act 1Solution
f1,2
m
f2,1
mKmg
M
Using FMa for bottom box
a mKmg/M
18
Inclined Plane with Friction
  • Draw free-body diagram

ma
?KN
j
N
?
mg
?
i
19
Inclined plane...
  • Consider i and j components of FNET ma

?KN
ma
j
N
?
a / g sin ?????Kcos ?
?
mg
mg cos ??
i
mg sin ??
20
Static Friction...
  • So far we have considered friction acting when
    the two surfaces move relative to each other-
    I.e. when they slide..
  • We also know that it acts in when they move
    togetherthe static case.
  • In these cases, the force provided by friction
    will depend on the OTHER forces on the parts of
    the system.

j
N
F
i
fF
mg
21
Static Friction(with one surface stationary)
  • Just like in the sliding case except a 0.
  • i F ??fF 0
  • j N mg
  • While the block is static fF ??F

j
N
F
i
fF
mg
22
Static Friction
  • The maximum possible force that the friction
    between two objects can provide is fMAX ?SN,
    where ?s is the coefficient of static
    friction.
  • So fF ? ?S N.
  • As one increases F, fF gets bigger until fF ?SN
    and the object starts to move.
  • If an object doesnt move, its static friction
  • If an object does move, its dynamic friction

j
N
F
i
fF
mg
23
Static Friction...
Suitcase
  • ?S is discovered by increasing F until the block
    starts to slide
  • i FMAX ???SN 0
  • j N mg
  • ?S ??FMAX / mg

j
N
FMAX
i
?Smg
mg
24
Lecture 7, Act 2Forces and Motion
  • A box of mass m 10.21 kg is at rest on a floor.
    The coefficient of static friction between the
    floor and the box is ms 0.4.
  • A rope is attached to the box and pulled at an
    angle of q 30o above horizontal with tension T
    40 N.
  • Does the box move?
  • (a) yes (b) no (c) too close to call

T

q
m
static friction (ms 0.4 )
25
Lecture 7, Act 2Solution
  • Pick axes draw FBD of box
  • Apply FNET ma

y N T sin q - mg maY 0
N
N mg - T sin q
T
q
m
fFR
x T cos q - fFR maX
ax will be positive (i.e. the box will move) if
T cos q gt fFR
mg
26
Lecture 7, Act 2Solution
y N 80 N
N
T
fMAX msN
q
m
mg
27
Halftime
28
Probability Puzzler
  • You are on a game show and there are three closed
    doors in front of you. Behind one door is a new
    car. Behind the other two are smelly old goats.
  • You pick door 1. Before opening your door the
    host opens door 2 and reveals a goat. He gives
    you the option of changing your guess to door 3.
    Should you switch to door 3?
  • Definitely Yes the odds of winning are better.
  • Definitely No the odds of winning are worse.
  • It makes no difference the odds of winning are
    the same either way.

29
  • Definitely Yes. The odds of winningdouble if you
    switch !!

3
2
1
Only Assumption The host always shows you a goat.
30
Static Friction
  • We can also consider ?S on an inclined plane.
  • In this case, the force provided by friction will
    depend on the angle ? of the plane.

?
31
Static Friction...
  • The force provided by friction, fF , depends on ?.

fF
ma 0 (block is not moving)
mg sin ????ff ???
N
?
(Newtons 2nd Law along x-axis)
mg
?
32
Static Friction...
Blocks
  • We can find ?s by increasing the ramp angle until
    the block slides

mg sin ????ff????
In this case, when it starts to slide
?ff????SN ? ??Smg cos ?M
?SN
mg sin ?M????Smg cos ?M????
N
mg
??M
?S???tan ?M?
?
33
Additional comments on Friction
  • Since fF ?N , kinetic friction does not
    depend on the area of the surfaces in contact.
  • By definition, it must be true that ?S ³ ?K
    for any system (think about it...).

34
Aside
  • Graph of Frictional force vs Applied force

fF ?SN
fF ?KN
fF
fF FA
FA
35
Problem Box on Truck
  • A box with mass m sits in the back of a truck.
    The coefficient of static friction between the
    box and the truck is ?S.
  • What is the maximum acceleration a that the
    truck can have without the box slipping?

?S
m
a
36
Problem Box on Truck
  • Draw Free Body Diagram for box
  • Consider case where fF is max...(i.e. if the
    acceleration were any larger, the box would
    slip).

N
j
i
fF ?SN
mg
37
Problem Box on Truck
  • Use FNET ma for both i and j components
  • i ?SN maMAX
  • j N mg
  • aMAX ?S g

N
j
aMAX
i
fF ?SN
mg
38
Lecture 7, Act 3Forces and Motion
  • An inclined plane is accelerating with constant
    acceleration a. A box resting on the plane is
    held in place by static friction. What is the
    direction of the static frictional force?

?S
a
Ff
Ff
Ff
(a) (b) (c)
39
Lecture 7, Act 3Solution
  • First consider the case where the inclined plane
    is not accelerating.

N
Ff
mg
40
Lecture 7, Act 3Solution
  • If the inclined plane is accelerating, the normal
    force decreases and the frictional force
    increases, but the frictional force still points
    along the plane

N
Ff
a
mg
41
Problem Putting on the brakes
Wheel
  • Anti-lock brakes work by making sure the wheels
    roll without slipping. This maximizes the
    frictional force slowing the car since ?S gt ?K
    .
  • The driver of a car moving with speed vo slams on
    the brakes. The coefficient of static friction
    between the wheels and the road is ?S . What is
    the stopping distance D?

42
Problem Putting on the brakes
  • Use FNET ma for both i and j components
  • i ?SN ma
  • j N mg
  • a ?S g

N
j
a
i
fF ?SN
mg
43
Problem Putting on the brakes
  • As in the last example, find ab ?Sg.
  • Using the kinematic equation v2 - v02 2a( x
    -x0 )
  • In our problem 0 - v02 ? 2ab( D )

vo
ab
v 0
D
44
Problem Putting on the brakes
  • In our problem 0 - v02 ? 2ab( D )
  • Solving for D
  • Putting in ab ?Sg

45
Recap of todays lecture
  • Friction
  • What is it?
  • How do we characterize it?
  • Model of friction.
  • Static Kinetic friction.
  • Some problems involving friction.
  • Box on truck.
  • Braking distance.
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