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Transcript
x(t 0) x0 Newton’s Laws of Motion, Friction and Inclined Planes 1. With no external force applied, a body will move with a constant dv m velocity v dt 2. mass x acceleration = sum of external forces* 3. If body A is in contact with body B and exerts a force upon it, the force upon A due to B is equal in magnitude and opposite in direction. Tension y x g 9.81ms 2 T a Normal R contact force m Friction F Weight mg Consider a block being pulled uphill via force T. The vector sum of forces results in an acceleration a directly up the hill. Surface contact is maintained at all times. Displacement A body is said to be in equilibrium if the vector sum of external forces is zero f i i x(t ) The force due to gravity upon a body of mass m is its weight and has magnitude mg, where g is the local gravitational field strength. dv d 2 x a dt dt 2 Velocity Acceleration y : 0 R mg cos ma T cos mg sin F 0 R T sin mg cos m mg sin mg cos Sliding friction model (friction always resists motion) x: y: mg sin R R mg cos x : 0 mg sin m R m Applying Newton Second Law in x and y directions F mR F mR Displacement Velocity and Acceleration are vector quantities Example 1: Block is on the point of sliding, T = 0. Note F will point in the opposite direction as the block will slide downhill if is increased. Rough inclined plane with coefficient of friction m between block of mass m and plane. x: y: dx v dt m tan y In equilibrium Sliding g 9.81ms 2 x ma T cos mg sin m R mg cos T sin R R F m 0 ma T cos mg sin m mg cos T sin T a cos m sin g sin m cos m *Actually Newton #2 states the rate of change of momentum = sum of the external forces. d mv dt mg fi If mass remains constant the LHS is mass x acceleration. i Mathematics topic handout: Forces, Friction and Newton’s Laws Dr Andrew French. www.eclecticon.info PAGE 1 Example 2: A block of 10kg is in equilibrium ‘at the point of sliding’ uphill (this is called limiting friction). If the plane is inclined at 30o and the tension is at 45o to the plane, what is T given a coefficient of friction of m = 1/5 ? 0 x: T 10 12 g 15 R 2 0 R y: Tension y x g 9.81ms 2 T 0 Normal R contact force T 5 g 15 R 2 45 o 10 T 3 T 10 g R 5g 3 2 2 2 Friction 30o F 30o T T 5 g 15 5 g 3 2 2 Weight 10g T 5 2 g g 6 15 T 6 5 T g 5 2 6 T 5 5 2 6 6 g Resolving forces y T 7.93 g 10 10 8 m 30o x 45o 3 3 max ma y 8 3 5 3 max 10 cos 30 3cos 45 2 o o ma y 10sin 30 3sin 45 8 3 3 2 o o The weight of the puss Mathematics topic handout: Forces, Friction and Newton’s Laws Dr Andrew French. www.eclecticon.info PAGE 2