View source for Friction

Claimed by Blake Castleman 11/23/2018 (Work in Progress)

This page discusses the concept of friction and how it relates to both moving and static objects.


==The Main Idea==
Friction is caused by the interactions between the atoms that make up objects. When objects interact, the atoms that make up the objects also interact. Temperatures of interacting surfaces rise because of such interactions. Friction is a force that resists movement. Generally, friction makes it harder to move objects. There are two main types of friction that are covered in Physics 2211: Static Friction and Kinetic Friction. Static friction can be described as the friction acting on resting objects. Kinetic friction is the friction acting on objects in motion. 

Frictional forces depend on a few factors: the normal force and the coefficient of friction. 

In simple terms, the normal force <math> {F}_{N} </math> or <math> {N} </math> is the equivalent force between objects. For example, when an object of mass '''M''' is placed on a table, there is a gravitational force '''Mg''' on the table. If the table can support the object without collapsing, the table exerts an equivalent force '''Mg''' on the object. According to the momentum principle, since there is no change in momentum, the net force must be '''0'''. This is also apparent since there is no movement if the table can support the object.

::<math> {p}_{f} - {p}_{i} = {F}_{net}{dt} = 0 </math>


OR

::<math> {F}_{g} = {M}{g} </math>
::<math> {N} = {M}{g} </math>
::<math> {F}_{net} = {F}_{g} - {N} = {0} </math>

The coefficient of friction is usually specific to each object or material. The coefficient of static friction is denoted by <math>{&mu;}_{s}</math> and the coefficient of kinetic friction is denoted by <math>{&mu;}_{k}</math> 


Static Friction:

::<math> {F}_{s} \le {&mu;}_{s}{N} </math>

Static friction is the frictional force that must be overcome to begin moving an object at rest. The static friction can be no more than the normal force multiplied by the coefficient of static friction. Therefore, the maximum static friction an object can have is <math> {&mu;}_{s}{N} </math>. 

Kinetic Friction:


::<math> {F}_{k} = {&mu;}_{k}{N} </math>

Kinetic friction is the frictional force that exists between objects already at motion. It acts to oppose the movement of an object. Kinetic friction can be observed, for example, when a soccer ball is kicked across a field. The friction between the ball and the field will eventually bring the ball to a stop.

Interestingly, friction is also required for rolling motion. Without friction, objects would not be able to roll. This is true because friction results in torque acting on the object, causing the rolling motion. An example of this can be seen in cars that are stuck in a ditch or similar situations. If there is not enough friction between the car's wheels and the ground, the car's wheels will simply spin in place, and the car will not move.

===A Mathematical Model===

As stated above:

Static Friction:

::<math> {F}_{s} \le {&mu;}_{s}{N} </math>

Kinetic Friction:

::<math> {F}_{k} = {&mu;}_{k}{N} </math>

When attempting to solve problems relating to friction, one possible method of approach is to consider the net force acting on an object. If there is a force <math> {F}</math> pushing an object to the right, and a frictional force <math>{F}_{f}</math> opposing the movement, then the net force is <math> {F}_{net} = {F} - {F}_{f} </math>.

Another possible approach is by using the momentum principle <math> {p}_{f} - {p}_{i} = {F}_{net}{dt} </math>. The momentum principle can help solve problems where you need to account for time, net force, or change in momentum.

===A Computational Model===

[[File:Friction.gif]]

Link: 
https://trinket.io/glowscript/76028c1809


Code: 
 def friction():
    from __future__ import division
    from visual import *
    from visual.graph import *

    mcart = 100
    mew = vector(2.9,0,0)

    track =  box(pos=vector(0,-0.05,0), size=vector(20.0,0.05,0.10), color=color.white)
    cart =  box(pos=vector(-10,0.25,0), size=vector(.5,0.6,0.03), color=color.blue)
    marker = box(pos = vector(2,0,0), size = vector(0,20,5), color = color.red)

    cart.v=vector(2.4,0,0)
    cart.p = mcart*cart.v
    F = vector(90,0,0)
    F2 = vector(-200,0,0)
    F3 = (mcart * mew)
    print(F3)

    deltat = 0.01
    t = 0

    while t < 5.02:

        if cart.pos.x < 2:
            cart.v = cart.p / cart.m
            Fnet = F
            cart.p = cart.p + Fnet*deltat
            cart.pos = cart.pos + (cart.p/mcart)*deltat

        else:
            
            cart.v = cart.p / cart.m
            Fnet = F-F3
            cart.p = cart.p + Fnet*deltat
            cart.pos = cart.pos + (cart.p/mcart)*deltat
            
        t = t + deltat
        rate(100)
        
    print(cart.pos)
    
 friction()

==Conceptualizing Friction==
===Why Friction Exists===
It's important to understand why friction exists. Imagine a brick laying at rest on a table as seen below:

(Insert: Brick at rest, macroscale)

Now, if we take a look at the brick on a molecular level rather than a macroscopic scale, we can see that electron repulsion between the brick's molecules and the ground keeps the brick on the surface of the ground so that the brick doesn't simply "sink" into the ground. Electron repulsion one of the primary reasons why surfaces in contact interact with each other.
Because, however, there is a force due to gravity on the brick, the electrons in the ground also must exert a force on the brick to establish a net force of zero. This force from the electrons is created from the "spring-like" motion of the electrons on the brick when it begins to sink into the ground. The atoms in the ground will be squished together, and because electron repulsion grows stronger as electrons are closer, the atoms will repel each other and create a "spring-like" force on the brick. Once an equilibrium of forces is established, the molecular scale of the brick will look something like this:

(Insert: Brick at rest, molecular level)

Thus, when the brick is pushed forward, it will have to quite literally make the ground sink to make way for its motion. The force that the atoms in the path ahead exert on the brick is what we know as friction and accounts for the reason why friction is dependent on the normal force.

(Insert: Brick accelerating, molecular level)

===Understanding Work Done by Friction===
As we know, the equation for work is as follows:

::<math> W = Fd </math>    (for constant forces and one dimensional motion)

When friction is brought into the equation therefore, we get:

::<math> W = fd </math>

We therefore should theoretically be able to calculate the work done by friction. However, we can observe an anomaly when we take into account the change in internal energy. Imagine a block moving at a constant velocity. Since the velocity is constant, the net force should be zero. If only an applied force and friction acts on the block, then the forces are equal.

::<math> \Sigma {F} = 0 = {F}_{app} - f </math>
::<math> {F}_{app} = f </math>

This means that if we move an object a distance d, then the total energy change of the system is zero since the forces are equal and d is the same variable in both instances:

::<math> \Delta {E}_{sys} = 0 = {F}_{app} d - fd </math>

However, in a real world scenario, we observe that the temperature of the block increases as the block moves along the surface. According to our equations however, this cannot be possible since the net energy change is zero. The block moves at constant velocity which means that there is no kinetic energy change and no energy is transferred from outside the system. How is this possible?
Looking at the block on a micro scale, it happens that the ground is actually not a perfect smooth surface. Instead, all surfaces have "teeth and gaps" that make it so that the block is not always in contact with the floor.

(Insert: Block in motion, micro level with teeth)

Applying this observation to our equations, the distance the apply force acts on the block stays the same; however, the distance that the frictonal force is applied on is drastically reduced. Therefore, our new equation for work (assuming constant forces) is:

::<math> \Delta {E}_{sys} = {F}_{app} d - f{d}_{eff} </math>      where <math> {d}_{eff} < d </math>

Since kinetic energy remains constant, we can conclude that:

::<math> \Delta {E}_{sys} = \Delta {E}_{int} </math>

Now, our internal energy change is accounted for which shows why our temperature change exists.

==Examples==

Be sure to show all steps in your solution and include diagrams whenever possible

===Simple===

A 100Kg box is placed on a flat table. The box does not move. The coefficient of static friction <math> {&mu;}_{s} = {.25} </math> and the coefficient of kinetic friction <math> {&mu;}_{k} = {.15} </math>.
Find the force of friction <math>{F}_{s}</math>.




Solution:

Since the box does not move, there is only static friction. The normal force is equivalent to the force due to gravity: <math> {F}_{N} = {F}_{g} = {100}{g} </math>. The static friction can be found by: <math> {F}_{s} = {&mu;}_{s}{F}_{N} </math>

<math> {F}_{s} = {.25}*{100}*{9.8} = {245.25} </math>

===Middling===

A cart of mass 3Kg moves across a track pushed by a fan which exerts <math> {F} = <3,0,1> </math>N with an initial velocity <math> {v}_{i} = <1,0,1>\frac{{m}}{{s}}</math> . Find the required coefficient of kinetic friction <math> {&mu;}_{k} </math> needed to bring the cart to a stop in 10 seconds.


Solution:

Use the momentum principle: <math>{p}_{f} - {p}_{i} = {F}_{net}{dt}</math> and <math>{F}_{f} = {&mu;}_{k}{N} </math>

The final velocity must be 0. The initial velocity, initial force, and time are given. 

<math>0- <3,0,3> = {F}_{net}*{10s}</math>

<math> {F}_{net} = <-0.3,0,-0.3> </math>

<math> {F}_{net} = {F} - {F}_{f} </math>

<math> <-0.3,0,-0.3>  = <3,0,1> - {F}_{f}</math>

<math>{F}_{f}  = <3.3,0,1.3> </math>

<math> {F}_{f} = <3.3,0,1.3> = {&mu;}_{k}{N} </math>

<math> {N} = {3Kg} * {<0,9.8,0>} = <0,29.43,0> </math>

<math> {&mu;}_{k} = \frac{{F}_{f}}{{N}} = \frac{{<3.3,0,1.3>}}{{0,29.43,0}} </math>

===Difficult===

Two blocks are stacked on top of one another on a frictionless surface. Block A is stacked on top of Block B. Block A has a mass of 2 Kg while Block B has a mass of 4 Kg. The coefficient of friction between the blocks is <math> {&mu;}_{s} = .35 </math>. Find the maximum amount of force that can be applied to Block A so that the blocks stay together.


Solution:

Momentum Principle:

<math> {p}_{f} - {p}_{i} = {F}_{net}{dt} </math>

We need to find the force of friction at its maximum to find the maximum amount of force that can be exerted on Block A. <math> {F}_{f} = {&mu;}_{s}{N} </math>

Forces on Block A:

<math> {F}_{A} - {F}_{f} </math>

Forces on Block B:

<math> {F}_{f} </math>

Since we want the blocks to move together, they must therefore have the same acceleration. 

<math> {F}_{A} - {F}_{f} = {2 Kg} * {a} </math>

<math> {F}_{f} = {4 Kg} * {a} </math>

<math> {F}_{A} - {F}_{f} = {2 Kg} * {a} </math>

Since they have the same acceleration, we can use the acceleration to solve for the force applied.

<math> {a} = \frac{{F}_{A} - {F}_{f}}{{2 Kg}} </math>

<math> {a} = \frac{{F}_{f}}{{4}}  </math>

<math>\frac{{F}_{A} - {F}_{f}}{{2 Kg}}= \frac{{F}_{f}}{{4 Kg}} </math>

<math>{F}_{A}= \frac{{3}}{{2}}{F}_{f} </math>

<math>{F}_{A}= \frac{{3}}{{2}} * {.35}*{6Kg}*{9.8} = {30.87}</math> N

==Connectedness==

Friction is an important topic to understand because it has many industrial implications. Since friction can cause increases in temperature when objects move, engineers who work with moving objects must understand and account for friction to ensure systems work properly. For example, car engines must have proper oil and lubricants to prevent parts from scraping together and wearing down. Mechanical engineers, aerospace engineers, and civil engineers must deal with friction and its impacts every day!

== See also ==



===External links===

Internet resources on this topic

Hyper Physics: http://hyperphysics.phy-astr.gsu.edu/hbase/frict.html#fri

PHET Simulation: https://phet.colorado.edu/en/simulation/friction

==References==
[1] Serway, Raymond A., and John W. Jewett. Physics for Scientists and Engineers. Boston, MA: Cengage Brooks/Cole, 2014. Print.

[2] Sherwood, Bruce A. Matter & Interactions. By Ruth W. Chabay. 4th ed. Vol. 1. N.p.: John Wiley & Sons, 2015. 45-50. Print. Modern Mechanics.



[[Category:Contact Forces]]