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h1. Static Friction {excerpt} If an object is at rest with respect to a surface, friction will attempt to resist efforts to start the object sliding along the surface. Friction has the goal of keeping the object static _with respect to the surface_. This [static friction] is a response force -- it provides just enough force to keep the object stationary, and no more. [Static friction|static friction] is characterized by a limiting value. When the net force attempting to create sliding motion exceeds a certain value, [static friction] will be unable to prevent motion. {excerpt} h3. Quantitative Model of Static Friction h4. The Limiting Size of Static Friction The basic characteristics of static friction are well approximated by the limit expression: {latex}
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Excerpt

The specific manifestation of friction which attempts to resist efforts to move an object that is currently at rest with respect to a surface. If possible, static friction provides just enough force to keep the object stationary, and no more. When the net force attempting to create sliding motion exceeds a certain limiting value proportional to the normal force exerted by the surface on the object, static friction will be unable to prevent motion.

Static Friction as a Force

The Limiting Size of Static Friction

The basic characteristics of static friction are well approximated by the limit expression:

Latex
\begin{large}\[ F_{s} \le \mu_{s} N\]\end{large}
{latex} where μ~s~ is the *coefficient of static friction*. The coefficient of static friction is a dimensionless number, usually less than 1.0 (but _not_ required to be less than

where μs is the coefficient of static friction. The coefficient of static friction is a dimensionless number, usually less than 1.0 (but not required to be less than 1.0).

Rough

or

sticky

surfaces

will

yield

larger

coefficients

of

friction

than

smooth

surfaces.

_

N

_

is

the

[

normal

force

]

exerted

on

the

object

_

by

the

surface

which

is

creating

the

friction

_

,

which

is

a

measure

of

the

strength

of

the

contact

between

the

object

and

the

surface.

h4.

Determining

the

Force

of

Static

Friction

To

determine

the

force

of

static

friction

on

an

object,

calculate

the

net

force

_

in

the

absence

of

any

friction

_

and

compare

it

to

the

limiting

value

of

the

friction

force.

If

the

maximum

static

friction

force

is

larger

than

the

net

force

in

the

absence

of

friction,

then

friction

will

provide

the

force

necessary

to

make

the

total

net

force

equal

zero

*

assuming

*

that

the

net

force

has

no

component

perpendicular

to

the

surface.

If,

however,

the

maximum

static

friction

force

is

_

less

_

than

the

net

force

in

the

absence

of

friction,

static

friction

will

*

not

apply

*

(it

will

not

provide

a

force).

Instead,

kinetic

friction

will

apply.

{

Note
}

It

is

very

important

to

remember

that

for

an

object

at

rest

on

a

surface

and

subject

to

*

no

*

forces

that

would

act

to

cause

sliding,

the

static

friction

force

will

be

*

zero

*

!

(The

object

will

not

move

without

friction,

so

friction

"has

no

job

to

do".){note}

do".)

Static Friction as Non-Conservative Work

The work done by static friction would seem to be obviously zero, since an object subject to static friction is required to be stationary. There is an important loophole, however, in the fact that the object is only required to be stationary with respect to the surface in order for static friction to apply. Thus, if the surface itself is moving, the object is moving as well! This loophole is relevant in problems where one object sits on another, e.g. a box on a truck bed or a block on a second block, etc. In these examples, static friction can be the sole force responsible for changing the horizontal motion of the box, the top block, etc. Thus, it must be the case that the friction can do work.

Info

There is at least one other major loophole that allows static friction to do work. Real objects like people and cars are actually deformable (they are not perfectly modeled as rigid bodies). Thus, a person can cause their center of mass to translate without moving their feet, and a car can move forward without translating the point of contact between the tires and the ground. In this way (when viewing the person or car as a single object) the force of static friction on the person's feet or the car's tires can be made to do work.

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