Chapter 6 Application of Newton’s Laws Dr. Jie Zou PHY 1151 Department of Physics 1 Outline Frictional Forces Kinetic friction Static friction Strings and Tension Connected objects Springs and Hooke’s Law for Spring Forces Circular Motion Dr. Jie Zou PHY 1151 Department of Physics 2 Frictional Forces The origin of friction: Even “smooth” surfaces have irregularities when viewed at the microscopic level. This type of roughness contributes to friction. Two types of friction: Kinetic friction Static friction Dr. Jie Zou PHY 1151 Department of Physics 3 Kinetic Friction Kinetic friction fk: The friction encountered when surfaces slide against one another with a finite relative speed. Direction of the force of kinetic friction: Kinetic friction fk acts to oppose the sliding motion at the point of contact between the surfaces. Magnitude of the force of kinetic friction: In general, the force of kinetic friction is found to be proportional to the magnitude of the normal force, N, or fk = kN. The constant of proportionality, k, is referred to as the coefficient of kinetic friction. Dr. Jie Zou PHY 1151 Department of Physics 4 Kinetic Friction: Example 1 Someone at the other end of the table asks you to pass the salt. You slide the 50.0-g salt shaker in their direction, giving it an initial speed of 1.15 m/s. (a) If the shaker comes to a rest with constant acceleration in 0.840 m, what is the coefficient of kinetic friction between the shaker and the table? Dr. Jie Zou PHY 1151 Department of Physics 5 Kinetic Friction: Example 2 A trained sea lion slides from rest with constant acceleration down a 3.0-mlong ramp into a pool of water. If the ramp is inclined at an angle of 23 above the horizontal and the coefficient of kinetic friction between the sea lion and the ramp is 0.26, how long does it take for the sea lion to make a splash in the pool? Dr. Jie Zou PHY 1151 Department of Physics 6 Static Friction Static friction fs: Static friction tends to keep two surfaces from moving relative to one another. There is an upper limit to the force that can be exerted by static friction, fs,max. fs,max = sN. The constant of proportionality is called s, the coefficient of static friction. Magnitude: The force of static friction, fs, can have any value between zero and fs,max. Direction: The direction of fs is parallel to the surface of contact, and opposite to the direction the object would move if there no1151 friction. Dr. Jiewere Zou PHY Department of Physics 7 Static Friction: Example A flatbed truck slowly tilts its bed upward to dispose of a 95.0-kg crate. For small angles of tilt the crate stays put, but when the tilt angle exceeds 23.3 the crate begins to slide. (a) What is the coefficient of static friction between the bed of the truck and the crate? (b) Find the magnitude of the static friction acting on the crate. Dr. Jie Zou PHY 1151 Department of Physics 8 Strings and Tension: Example To hang a 6.20 kg pot of flowers, a gardener uses two wires-one attached horizontally to a wall, the other sloping at an angle of = 40.0 and attached to the ceiling. Find the tension in each wire. Dr. Jie Zou PHY 1151 Department of Physics 9 Springs and Hooke’s Law (Ideal) Springs and Hooke’s Law Magnitude of the spring force: The spring force is proportional to the amount, x, by which it is stretched or compressed. Direction of the spring force: Opposite to the displacement from the equilibrium length of the spring. Hooke’s Law: F = - k x. k: Force constant of the spring, units: N/m. x: displacement from the equilibrium length of the spring Dr. Jie Zou PHY 1151 Department of Physics 10 Springs and Hooke’s Law: Example A 1.50-kg object hangs motionless from a spring with a force constant k = 250 N/m. How far is the spring stretched from its equilibrium length? Dr. Jie Zou PHY 1151 Department of Physics 11 Connected Objects A block of mass m1 slides on a frictionless tabletop. It is connected to a string that passes over a pulley and suspends a mass m2. Find (a) the acceleration of the masses and (b) the tension in the string. Dr. Jie Zou PHY 1151 Department of Physics 12 Circular Motion Centripetal acceleration, acp: Newton’s 2nd Law applied to circular motion: To make an object move in a circle with constant speed, a force must act on it that is directed toward the center of the circle. Direction: Directed toward the center of the circle Magnitude: acp = v2/r, where v = speed and r = radius The centripetal force is proportional to the centripetal acceleration. fcp = macp Centripetal force, fcp: Direction: Directed toward the center of the circle Magnitude: fcp = macp = mv2/r Dr. Jie Zou PHY 1151 Department of Physics 13 Circular Motion: Example A 1200-kg car rounds a corner of radius r = 45 m. If the coefficient of static friction between the tires and the road is s = 0.82, what is the greatest speed the car can have in the corner without skidding? Dr. Jie Zou PHY 1151 Department of Physics 14 Homework See online homework assignment at www.masteringphysics.com Hand-written homework assignment: Chapter 6, Page 178, Problems: #10 Dr. Jie Zou PHY 1151 Department of Physics 15