Friction & Air Resistance

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Last updated 8:07 PM on 9/26/26
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17 Terms

1
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whenever an object moves or attempts to move on a surface, there is a force

parallel to the surface in the opposite direction to the motion or attempt at motion

  • this is known as friction


2
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if an object is attempting to move, the frictional force is

static friction

3
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if an object is already moving, the frictional force is

kinetic friction

4
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static friction

if an object is pushed with an increasing force, the force of static friction fs will increase to exactly balance the applied force

  • the object thus does not accelerate, and the acceleration = 0 and thus Fnet = 0 by Newton’s 2nd law of Fnet = ma

  • the static friction force fs is equal and opposite to the applied force Fa if the object does not move


5
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at fs,max, the acceleration of the object is

a > 0 and thus Fnet > 0, and the object is still at rest and thus its velocity v = 0, but it is about to move

  • an object will begin to slide if the applied force is increased beyond fs,max


6
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when the applied force exceeds the maximum possible static friction fs,max, the object will

begin to move from rest (v = 0)

  • a > 0, Fnet > 0


7
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static friction force and coefficient

  • for an object that is not slipping: fs = -Fa, and fs < fs,max

  • for an object that is on the verge of slipping: fs = fs,max = us N

    • fs,max is proportional to the normal force (N) that the bottom surface exerts on the top surface

    • us is the proportionality constant of static friction


8
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origin of friction occurs from

a few contact points between the top and bottom surface which hinders the sliding of two objects against each other

  • a larger force needs to be applied to overcome the contact points, and the magnitude of the force depends on the height of the peaks and valleys (roughness of the surfaces)


9
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the coefficient of static friction, us, depends on the

roughness of the two surfaces in contact

  • it is thus a ratio between two surfaces, and is dimensionless

  • ex. wood on wood, rubber on asphalt, metal on ice


10
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when fs < fs,max, the static friction does not depend on

the static friction coefficient us at all

  • the coefficient us only matters when the object is on the verge of slipping, and thus fs = fs,max


11
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kinetic friction fk is the

frictional force parallel to the surface that opposes the motion of a moving object

  • fk = uk N, and thus the force of kinetic friction fk is proportional to the normal force (N)

  • the kinetic friction coefficient uk depends on the roughness of the two surfaces in temporary contact

  • independent of the pushing / pulling force Fa

    • fs,max is greater than fk, which is constant (fk < fs,max)

    • uk < us


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it is generally harder to make an object slide starting from

rest than it is to keep making it slide

13
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the force of kinetic friction, fk, is

  • independent of the contact area between surfaces

  • approximately independent of the speed, as long as the speed is not too large


14
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air resistance (drag)

always points in the opposite direction of motion and is dependent on velocity / speed

  • its magnitude is Fd = ½ CApv²

    • C: streamline coefficient (shape dependent)

    • A: cross-sectional area of the object

    • p: density of air (1 kg / m³)

    • v: speed of the object


15
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motion in the presence of air resistance is

not at a constant acceleration, but it is at the very acceleration until it reaches the terminal velocity, from which point on it falls with constant velocity (a = 0)

  • this is when the force of air resistance (Fd) matches the gravitational force of the Earth on the object (mg)

    • Fnet = 0 (equal and opposite forces) and thus a = 0 (constant terminal velocity)


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terminal velocity

any object falling in air will eventually reach a terminal velocity when air resistance is equal and opposite to the gravitational force driving the fall

  • applying Newton’s 2nd law: ½ CApvt² - mg = 0, thus vt² = 2mg / CAp, and thus vt = √2mg / CAp


17
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terminal velocity vt is proportional to

√m and inversely proportional to √A

  • if the cross-sectional area of the object is increased, the terminal velocity is decreased

  • if the mass of the object is increased, the terminal velocity will be reached later during the fall and will therefore have a larger magnitude