Week 5 Applications of Newton's Laws Dr Sohail Amjad Outline Free-Body diagrams Applying Newton's First Law: Equilibrium Applying Newton's Second Law:Dynamics Frictional Forces Dynamics of Circular Motion Fundamental forces of Nature 2 / 29 Free-Body diagrams Newton's rst and second laws apply to a specic body. ΣF~ = 0 for an equilibrium ~ ΣF = m~a , for a non-equilibrium Whenever you use Newton's rst law, situation or Newton's second law, situation, you must decide at the beginning to which body you are referring. Only forces acting on the body matter. Free-body diagrams are essential to help identify the relevant forces. A free-body diagram is a diagram showing the chosen body by itself, free of its surroundings, with vectors drawn to show the magnitudes and directions of all the forces applied to the body by the various other bodies that interact with it. 3 / 29 Free-Body diagrams 4 / 29 Free-Body diagrams 5 / 29 Free-Body diagrams 6 / 29 Free-Body diagrams 7 / 29 Free-Body diagrams 8 / 29 Free-Body diagrams 9 / 29 Applying Newton's First Law - Equilibrium A body is in equilibrium when it is at rest or moving with constant velocity in an inertial frame of reference. For now, we will consider only equilibrium of a body that can be modeled as a particle. When a particle is in equilibrium, the net force acting on it (the vector sum of all the forces acting on it) be zero: ΣF~ = 0 We can also use the component form: ΣFx = 0, ΣFy = 0 10 / 29 Example A gymnast with mass suspends herself from the lower end of a hanging rope of negligible mass mG = 50.0 kg . The upper end of the rope is attached to the gymnasium ceiling. (a) What is the gymnast's weight? (b) What force (magnitude and direction) does the rope exert on her? (c) What is the tension at the top of the rope? 11 / 29 Example A gymnast with mass suspends herself from the lower end of a hanging rope of negligible mass mG = 50.0 kg . The upper end of the rope is attached to the gymnasium ceiling. (a) What is the gymnast's weight? (b) What force (magnitude and direction) does the rope exert on her? (c) What is the tension at the top of the rope? 12 / 29 Example a) wG = mG g = 50kg × 9.8m/s2 = 490 N b) ΣFy = 0 =⇒ TR on G + (−wG ) = 0 =⇒ TRo nG = wG = 490N c) Your answers? 13 / 29 Example A gymnast with mass suspends herself from the lower end of a hanging rope of negligible mass mG = 50.0 kg . The upper end of the rope is attached to the gymnasium ceiling. (a) What is the gymnast's weight? (b) What force (magnitude and direction) does the rope exert on her? (c) What is the tension at the top of the rope? Solve the problem if weight of Rope is 120 N . 14 / 29 Example A car engine with weight w hangs from a chain that is linked at ring O to two other chains, one fastened to the ceiling and the other to the wall. Find expressions for the tension in each of the three chains in terms of w. The weights of the ring and chains are negligible compared with the weight of the engine. 15 / 29 Example A car engine with weight w hangs from a chain that is linked at ring O to two other chains, one fastened to the ceiling and the other to the wall. Find expressions for the tension in each of the three chains in terms of w. The weights of the ring and chains are negligible compared with the weight of the engine. 16 / 29 Example A car engine with weight w hangs from a chain that is linked at ring O to two other chains, one fastened to the ceiling and the other to the wall. Find expressions for the tension in each of the three chains in terms of w. The weights of the ring and chains are negligible compared with the weight of the engine. T1 = w T3 = 1.2w T2 = 0.58w 17 / 29 Example A car of weight w rests on a slanted ramp attached to a trailer. Only a cable running from the trailer to the car prevents the car from rolling o the ramp. (The car's brakes are o and its transmission is in neutral.) Find the tension in the cable and the force that the ramp exerts on the car's tires. 18 / 29 Example A car of weight w rests on a slanted ramp attached to a trailer. Only a cable running from the trailer to the car prevents the car from rolling o the ramp. (The car's brakes are o and its transmission is in neutral.) Find the tension in the cable and the force that the ramp exerts on the car's tires. 19 / 29 Example ΣFx = T + (−wsinα) = 0 =⇒ T = w sinα ΣFy = n + (−wcosα) = 0 =⇒ n = w cosα 20 / 29 Applying Newton's Second Law Non-Equilibrium Let's discuss dynamics (opposed to statics - not kinematics) problems. In these problems, we apply Newton's second law to bodies on which the net force is not zero. These bodies are not in equilibrium and hence are accelerating. The net force on the body is equal to the mass of the body times its acceleration: ΣF~ = m~a We can also use the component form: ΣFx = max , ΣFy = may 21 / 29 Example An iceboat is at rest on a frictionless horizontal surface. A wind is blowing along the direction of the runners so that 4.0 s after the iceboat is released, it is moving at 6 m/s. What constant horizontal force FW does the wind exert on the iceboat? The combined mass of iceboat and rider is 200 kg. 22 / 29 Example An iceboat is at rest on a frictionless horizontal surface. A wind is blowing along the direction of the runners so that 4.0 s after the iceboat is released, it is moving at 6 m/s. What constant horizontal force FW does the wind exert on the iceboat? The combined mass of iceboat and rider is 200 kg. FW = 300 N 23 / 29 Example Let's complicate things a bit An iceboat is at rest on a frictionless horizontal surface. A wind is blowing along the direction of the runners so that 4.0 s after the iceboat is released, it is moving at 6 m/s. What constant horizontal force FW does the wind exert on the iceboat? The combined mass of iceboat and rider is 200 kg. Suppose a constant horizontal friction force with magnitude 100 N opposes the motion of the iceboat. In this case, what constant force FW must the wind exert on the iceboat to cause the same constant x-acceleration ax = 1.5 m/s2 ? 24 / 29 Example An iceboat is at rest on a frictionless horizontal surface. A wind is blowing along the direction of the runners so that 4.0 s after the iceboat is released, it is moving at 6 m/s. What constant horizontal force FW does the wind exert on the iceboat? The combined mass of iceboat and rider is 200 kg. Suppose a constant horizontal friction force with magnitude 100 N opposes the motion of the iceboat. In this case, what constant force FW must the wind exert on the iceboat to cause the same constant x-acceleration ax = 1.5 m/s2 ? FW = 400 N 25 / 29 Example An elevator and its load have a combined mass of 800 kg . The elevator is initially moving downward at 10 m/s it slows to a stop with constant acceleration in a distance of What is the tension T 25.0 m. in the supporting cable while the elevator is being brought to rest? 26 / 29 Example 800 kg . The elevator 10 m/s it slows to a stop with constant 25.0 m. What is the tension T in the An elevator and its load have a combined mass of is initially moving downward at acceleration in a distance of supporting cable while the elevator is being brought to rest? T = 9440 N . 27 / 29 Example Let's complicate things a bit .... 800 kg . The elevator 10 m/s it slows to a stop with constant 25.0 m. What is the tension T in the An elevator and its load have a combined mass of is initially moving downward at acceleration in a distance of supporting cable while the elevator is being brought to rest? A 50.0-kg woman stands on a bathroom scale while riding in the elevator. What is the reading on the scale? 28 / 29 Example Let's complicate things a bit .... 800 kg . The elevator 10 m/s it slows to a stop with constant 25.0 m. What is the tension T in the An elevator and its load have a combined mass of is initially moving downward at acceleration in a distance of supporting cable while the elevator is being brought to rest? A 50.0-kg woman stands on a bathroom scale while riding in the elevator. What is the reading on the scale? 390 N . Note: Real weight of woman = 490 N Apparent weight of woman when elevator is slowing down = 590 N 29 / 29