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Physics 2211: Lecture 11 Todays Agenda

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How do we characterize this in terms we have learned? Friction results in a force in the direction opposite to the direction of motion! ... – PowerPoint PPT presentation

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Title: Physics 2211: Lecture 11 Todays Agenda


1
Physics 2211 Lecture 11Todays Agenda
  • Friction
  • What is it?
  • How do we characterize it?
  • Model of friction
  • Static Kinetic friction
  • Some problems involving friction

2
New Topic Friction
  • What does it do?
  • It opposes motion!
  • How do we characterize this in terms we have
    learned?
  • Friction results in a force in the direction
    opposite to the direction of motion!

y
x
3
Friction...
  • Friction is caused by the microscopic
    interactions between the two surfaces
  • Friction force is the result of the
    electromagnetic forces acting between the two
    surfaces.

4
Friction...
  • Force of friction acts to oppose motion
  • Parallel to surface.
  • Perpendicular to Normal force.

y
x
5
Model for Sliding Friction
  • The direction of the frictional force vector is
    perpendicular
  • to the normal force vector .
  • The constant ?K is called the coefficient of
    kinetic friction.

6
Model...
  • Dynamics
  • SFX FA ? ?KN ma
  • SFY N mg
  • so FA ???Kmg ma

y
Assume forces are acting at center of mass of
block.
x
7
Example Forces and Motion
  • A box of mass m1 1.5 kg is being pulled by a
    horizontal string having tension T 90 N. It
    slides with friction (mk1 0.51) on top of a
    second box having mass m2 3 kg, which in turn
    slides with friction (mk2 0.068) on a floor.
  • What is the acceleration of the second box (m2) ?

slides with friction (mk10.51 )
T
m1

slides with friction
(mk20.068 )
a ?
m2
8
Example Forces and Motion
  • First draw FBD of the top box

N1
m1
fK1 - mK1N1
T
y
- m1g
x
9
Example Forces and Motion
  • Newtons 3rd law says the forces on box 1 exerted
    by box 2 are equal and opposite to the forces on
    box 2 exerts by box 1.
  • As we just saw, these forces are due to friction
    and the normal force.

N1 m1g
- mK1m1g
m1
fK1
m2
- fK1
- N1
10
Example Forces and Motion
  • Now consider the FBD of box 2

N2
fK1 mk1m1g
m2
fK2 mk2N2
-N1 -m1g
-m2g
11
Inclined Plane with Friction
  • Draw free-body diagram

a
y
?
x
12
Inclined plane...
  • Resolve force due to gravity into components.
  • Applied Newtons 2nd law in both dimensions.

y
x
13
Static Friction...
  • So far we have considered friction acting when
    something moves.
  • We also know that it acts in un-moving static
    systems
  • In these cases, the force provided by friction
    will depend on the forces applied on the system.

y
x
14
Static Friction...
  • Just like in the sliding case except a 0.
  • x FA ??fF 0
  • y N mg
  • While the block is static fF ??FA

y
x
15
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.

y
x
16
Static Friction...
  • ?S is discovered by increasing F until just
    before the block starts to slide
  • x FMAX ?? fMAX 0 but fMAX ?SN
  • y N mg
  • ?S ??FMAX / mg

y
x
17
Example Forces 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?

T

q
m
static friction (ms 0.4 )
18
Example Forces and Motion
  • Pick axes draw FBD of box.

y N T sin q - mg maY 0
N mg - T sin q
x T cos q - fF maX
m
The box will move if T cos q - fF gt 0
19
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.

?
20
Static Friction...
  • The force provided by friction, fF , depends on ?.

fF
N
a 0 (block is not moving)
mg sin ????fF ???
?
(Newtons 2nd Law along x-axis)
mg
?
21
Static Friction...
  • We can find ?s by increasing the ramp angle until
    the block slides

mg sin ?M ???fF????
fF
N
In this case
?fF????SN ? ??Smg cos ?M
mg sin ?M????Smg cos ?M????
?M
mg
?
?S???tan ?M?
22
Additional comments on Friction
  • Since fF ?N , the force of friction does not
    depend on the area of the surfaces in contact.
  • By definition, it must be true that ?S gt ?K
    for any system (think about it...).

23
Aside
  • Graph of Frictional force vs Applied force

fF ?SN
fF ?KN
fF
fF FA
FA
24
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
25
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
y
fF ?SN
x
mg
26
Problem Box on Truck
  • Use for both x and y
    directions
  • x ?SN maMAX
  • y N mg
  • aMAX ?S g

N
y
aMAX
fF ?SN
x
mg
27
Lecture 11, ActForces 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)
28
Recap of todays lecture
  • Friction
  • What is it?
  • How do we characterize it?
  • Model of friction.
  • Static Kinetic friction.
  • Some problems involving friction.
  • Read Sections 5.2 in Tipler.
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