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Lecture notes for Physics 1, Friction.
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FRICTION
Friction – a force that always acts to resist the motion of one object sliding on another.
Principles of Friction
Frictional force is unchanged whether the object lies on its side or bottom.
F (^) s max N
Normal force (N) – the force exerted by the surface to the object placed to it. This force is always perpendicular to the surface.
s = fs max N where :
- coefficient of friction ff – frictional force fs – static friction fk – kinetic friction N – normal force
Solution:
Since the speed is constant, the total force acting on the body is equal to zero.
F = 0
horizontal forces vertical forces
Fx = 0 Fy = 0
Fa + (-)ff = 0 N + (-)w = 0
Fa = ff N = w
w = mg = (40kg) (9.8 m/s^2 = 392 kg m/s^2 or N
A. k = ff = fs ; deriving the formula of static friction, we obtain N N
fs = k N
= (0.5) (392 N)
= 196 N since fs = Fa, the force needed to start the object moving is 196 N.
B. Fk = k N
= (0.3) (392 N)
= 117.6 N ; therefore to keep the object moving a force of 117.6N is needed at constant speed.
Problem #2: A block is pulled to the right at constant velocity by a force of 10 N acting 30^0 above the horizontal. The coefficient of sliding friction between the block and the surface is 0.5. What is the weight of the block?
N Fa = 10 N
Fk 3 = 30^0
k = 0.
w =?
Since weight is unknown, all forces acting in the system vertically must be known. First, the must calculate components of applied force.
Fax = cos Fay = sin Fa Fa Fax = Fa cos Fay = Fa sin
Fx = 0 Fy = 0
Fax + (-)fk = 0 N + (-)w + Fay = 0
Fax = fk w = N +Fay
Fa cos = fk w = N + Fa sin
Fa = 300 N
m = 50kg
ff θ
θ =30^0 w
Horizontal component of weight
wx = w sin
Vertical component of weight
wy = w cos
Fx = 0 Fy = 0
F + (-)ff +(-) wx = 0 N + (-)wy = 0
F - wx = ff wy = N
F - w sin = ff w cos = N k = ff N
(^) f = F - w sin w cos = 300N – ( 490N) (sin 30^0 ) (490N) (cos 30^0 )
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