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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
if an object is attempting to move, the frictional force is
static friction
if an object is already moving, the frictional force is
kinetic friction
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
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
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
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
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)
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
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
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
it is generally harder to make an object slide starting from
rest than it is to keep making it slide
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
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
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)
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
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