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6 Applications of Newton’s Laws 6-1 Frictional Forces What is friction? To slide one such surface across another requires a force large enough to overcome the resistance of microscopic hills and valleys bumping together.
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Kinetic Friction For an object moving : coefficient of kinetic friction; independent of area N: Normal force µk=µk= Ski on snow 0.05 Wood on leather 0.4 Rubber on concrete 0.8
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Properties of kinetic frictional force Opposes motion in direction of surface Depends on smooth of surface Increase as force pressing surface increasing
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How do we apply ? x y
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Ex. Driving at 12 m/s slow on brake, m=1000kg, the coefficient µ k is 0.8, what is the acceleration? How long to stop?
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Static Friction For a stationary object V=0 Object is static, until F>f s(max) object starts motion coefficient of static friction µs=µs= Ski on snow 0.1 Wood on leather 0.5 Rubber on concrete 1-4
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Independent of the area of contact Static friction is not relative with the normal force, (direction and magnitude), except f s(max) Direction of f s is parallel to the surface of contact, and opposite to the direction the object would move if there were no friction, (opposite to the direction of the tendency of motion)
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θ x y Change the tilt angle θ, let the static friction get the maximum value, but the box still rest, find the coefficient of static friction?
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