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Chapter 4 Dynamics: Newton’s Laws of Motion The Tension Force Example: A window washer standing in a bucket pulls herself up with a rope over a pulley as shown. The bucket+window washer have a combined mass of 65 kg. Starting from rest at the bottom, how much constant force must she exert on the rope to reach a window 160 m above her in one-half of a minute? +y T T ! ay m= 65 kg 160 m W ∑F y = 2T − W = may The Tension Force ∑F y mg = 2T − W = may ⇒T = m ( ay + g) 2 Find ay using constant acceleration equation: y = v0 y t + ay t 1 2 2 y = 160 m, v0 y = 0, t = 30 s 2y 2(160) 2 y = 0 + ay t ⇒ ay = 2 = = 0.36 m/s 2 t 30 m(ay + g) 65(0.36 + 9.80) ∴T = = = 330 N 2 2 ≈ 74 lbs 1 2 2 Types of Forces: An Overview Examples of Nonfundamental Forces -All of these are derived from the electroweak force: normal or support forces friction tension in a rope Static and Kinetic Frictional Forces When an object is in contact with a surface there is a force acting on that object. The component of this force that is parallel to the surface is called the frictional force. The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may have been corrupted. Restart your computer, and then open the file again. If the red x still appears, you may have to delete the image and then insert it again. “cold welds” Static and Kinetic Frictional Forces When the two surfaces are not sliding across one another the friction is called static friction. The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may have been corrupted. Restart your computer, and then open the file again. If the red x still appears, you may have to delete the image and then insert it again. Static and Kinetic Frictional Forces The magnitude of the static frictional force can have any value from zero up to a maximum value. fs ≤ f f MAX s 0 < µs < 1 MAX s = µ s FN Not a vector equation! fS is parallel to the surface, FN is perpendicular to the surface. is called the coefficient of static friction. Static and Kinetic Frictional Forces Note that the magnitude of the frictional force does not depend on the contact area of the surfaces. The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may have been corrupted. Restart your computer, and then open the file again. If the red x still appears, you may have to delete the image and then insert it again. Static and Kinetic Frictional Forces Static friction opposes the impending relative motion between two objects. Kinetic friction opposes the relative sliding motion that actually does occur. f k = µ k FN 0 < µ ks < 1 is called the coefficient of kinetic friction. Static and Kinetic Frictional Forces The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may have been corrupted. Restart your computer, and then open the file again. If the red x still appears, you may have to delete the image and then insert it again. Usually, µs > µk Static and Kinetic Frictional Forces Example. A sled and a rider are moving at a speed of 4.0 m/s along a horizontal stretch of snow. The snow exerts a kinetic frictional force on the runners of the sled, so the sled slows down and eventually comes to a stop. The coefficient of kinetic friction is 0.050 and the mass of the sled and rider is 40 kg. Find the kinetic frictional force and the displacement, x, of the sled. The image cannot be displayed. Your computer may not have enough memory to open the image, or the image may have been corrupted. Restart your computer, and then open the file again. If the red x still appears, you may have to delete the image and then insert it again. Static and Kinetic Frictional Forces 1. Use Newton’s 2nd law in x and y directions. ΣFx = -fk = max --> ax = -fk/m = -µkFN/m (since fk = µkFN) ΣFy = FN - W = FN - mg = may = 0 --> FN = mg fk = µkFN = µkmg = (0.050)(40)(9.8) = 20 N Static and Kinetic Frictional Forces ax = -µkFN/m = -µkmg/m = -µkg = -(0.050)(9.8) = -0.49 m/s2 2. Solve for x using ax and kinematic equations. x ? v0x 4.0 m/s vx 0 m/s ax -0.49 m/s2 t independent vx2 = v0x2 + 2axx --> x = (vx2 - v0x2)/(2ax) of mass of 2 2 = (0 - 4.0 )/(2(-0.49)) = 16 m sled+rider Example. Block 1 (mass m1 = 8.00 kg) is moving on a 30.0o incline with a coefficient of kinetic friction between the block and incline of 0.300. This block is connected to block 2 (mass m2 = 22.0 kg) by a massless cord that passes over a massless and frictionless pulley. Find the acceleration of each block and the tension in the cord. fk fk fk m1 = 8.00 kg m2 = 22.0 kg Find a, T and T’ µk = 0.300 Block 1: Σ Fx = -fk - W1 sin 30.0o + T = m1a fk Σ Fy = FN - W1 cos 30.0o = 0 è FN = W1 cos 30.0o Block 2: Σ Fy = T’ - W2 = m2(-a) We also know: T = T’ since the pulley and cord are massless fk = µkFN = µkm1g cos 30.0o = (0.300)(8.00)(9.80)(0.866) = 20.4 N Equations we’re left with to solve for a and T: -fk - W1 sin 30.0o + T = m1a T - W2 = -m2a è T = W2 - m2a Substituting for T in the first equation: -fk - W1 sin 30.0o + W2 - m2a = m1a a = (-fk - W1 sin 30.0o + W2)/(m1 + m2) = (-20.4 - (8.00)(9.80)(0.500) + (22.0)(9.80))/(8.00 + 22.0) = 5.20 m/s2 T = W2 - m2a = (22.0)(9.80) - (22.0)(5.20) = 101 N