Newton’s Third Law of Motion Physics 111 Lecture 9 (Walker: 5.4-5) Forces always come in pairs, acting on different objects: Newton’s Third Law Free Body Diagram Solving 2-D Force Problems Weight & Gravity If Object 1 exerts a force F on Object 2, then Object 2 exerts a force –F on Object 1. These forces are called action-reaction pairs. Alternate Wording: Sept. 21, 2009 “For every action there is an equal and opposite reaction.” r r FA on B = − FB on A Quiz Wednesday - Chaps. 3 & 4 Lecture 9 1/26 Question Lecture 9 2/26 Applying Newton’s Laws • Assumptions – Objects behave as particles Small car is pushing large truck that has a dead battery. Mass of truck is much larger than mass of car. Which of the following statements is true? • can ignore rotational motion (for now) a. Car exerts force on truck, but truck doesn’t exert force on car. b. Car exerts a larger force on truck than truck exerts on car. c. Car exerts the same force on truck as truck exerts on car. d. Truck exerts a larger force on car than car exerts on truck. e. Truck exerts a force on car, but car doesn’t exert a force – Masses of strings or ropes are negligible – Interested only in the forces acting on the object • can neglect reaction forces • Start with a Free Body Diagram on truck. Lecture 9 3/26 Lecture 9 4/26 Free Body Diagram (FBD) Example of a free-body diagram: • Diagram that shows all force vectors acting on the object of interest. How to construct: – Draw object as a dot (point particle) – Replace everything that touches object with appropriate force vectors – Add weight vector (always points straight down) – Choose a convenient coordinate system – Resolve force vectors into components Lecture 9 5/26 6/26 Example 5-4 A box of mass m1=10.0 kg rests on a floor next to a box of mass m2=5.00 kg. If you push box 1 with a horizontal force of magnitude F=20.0N in the positive x-direction, (a) what is the acceleration of the boxes; (b) What is the magnitude of contact force F1? Of F2 ? Drawing Force Vectors Lecture 9 Lecture 9 7/26 Lecture 9 8/26 N F W FBD Combined Boxes N1 F1 y N2 F W1 FBD Box 1 Moving a Satellite (Deep Outer Space) F2 x W2 FBD Box 2 Only x acceleration in each case (y forces cancel) Combined Boxes: ax = F/(m1+m2) = 20N/15kg = 1.33 m/s2 Box 1: a1x = ax = (F - F1)/m1 so 1.33 m/s2 = (20N - F1)/10kg Thus F1 = 6.7 N Box 2: a2x = ax = F2/5kg so 1.33 m/s2 = F2/5kg Thus F2 = 6.7 N (as expected from Third Law !!) Lecture 9 9/26 Lecture 9 10/26 2D Newton’s 2nd Law Problems • Draw FBD and choose good coordinate system • Get force components: Fx = Fcosθ; Fy = Fsinθ • Use Newton 2nd Law ∑ F = ma in component form (treat x & y separately) ∑F x ∑F = ma x y = ma y • ax or ay may be zero Lecture 9 11/26 Lecture 9 12/26 F2 = 41N @ 52° CCW from x-ax F2x = F2 cos 52° = 25.2 N Finding Acceleration • ax = Fx/m = 51.2N / 940kg = 0.054 m/s2 • ay = Fy/m = 32.3N / 940kg = 0.034 m/s2 F2y = F2 sin 52° = 32.3 N F1x = 26 N F1y = 0 a = a x2 + a 2y = 0.064m / s 2 Net force: Fx = F1x + F2x = 26 N + 25.2 N = 51.2 N θ a = arctan⎜⎜ Fy = 32.3 N F = Fx2 + Fy2 = 60.5 N ⎛ Fy ⎞ ⎟⎟ = 32.2° ⎝ Fx ⎠ 13/26 ⎛ ay ⎞ ⎟⎟ = 32.2° ⎝ ax ⎠ • Note, also, a = Fnet/m and the angle of the acceleration is same as net force angle θ = arctan⎜⎜ Lecture 9 Newton proposed that every object in the universe attracts every other object with a force that has the following properties: The falling box is pulled toward Earth by long-range force of gravity. The gravitational pull on an object on or near the surface of the Earth is called weight, for which we use the symbol W. W = mg 14/26 Newton’s Law of Gravity* Weight Weight force is the entire Earth pulling on an object. Weight acts equally on objects at rest or in motion. The weight vector always points vertically downward, and it can be considered to act at the center of mass of the object. Lecture 9 1. The force is inversely proportional to the square of the distance between the objects. 2. The force is directly proportional to the product of the masses of the two objects. W g = 9.80 N/kg = 9.80 m/s2 down Lecture 9 15/26 Lecture 9 16/26 The Earth’s Gravitation* Newton’s Law of Gravity* F1 on 2 What is the gravitational force on an object of mass m at the surface of the Earth? The center of the Earth is one Earth radius (RE) away, so that is the distance r: mm = F2 on 1 = G 1 2 2 r G = 6.673 × 10−11 N m /kg 2 2 Therefore, r is distance between mass m1 and mass m2. where Direction of force on m1 is toward m2; direction of force on m2 is toward m1 (third law pair ! ) GM E RE2 g = 9.80 N/kg = 9.80 m/s2 Lecture 9 17/26 Lecture 9 18/26 Weight & Free Fall Earth Gravitation vs. Altitude* The acceleration of gravity decreases slowly with altitude: GM E g ( h) = ( RE + h) 2 GM E g (0) = = 9.83 m/s 2 RE 2 Lecture 9 g= 19/26 Weight of box of mass m is W = mg g = 9.80 N/kg = 9.80 m/s2 down ∑ Fy = −mg By Newton’s 2nd Law m may = -mg ay = -g = -9.80 m/s2 y Lecture 9 W 20/26 Apparent Weight Apparent Weight Your perception of your weight is based on the contact forces between your body and your surroundings. Elevator not accelerating: Wa=mg If your surroundings are accelerating, your apparent weight may be more or less than your actual weight. Elevator accelerates up: Wa> mg Elevator accelerates down: Wa< mg Force felt from contact with the floor (or a scale, etc.) in an accelerating system. Lecture 9 21/26 Apparent Weight (Example 5.7 from Walker) Lecture 9 22/26 Weight Components on Inclined Surface m = 5.0 kg a) Wa (at rest)? b) Wa ? (a =2.5m/s2 up) c) Wa ? (a =3.2 m/s2 down) Lecture 9 23/26 Lecture 9 24/26 Force Component Down Inclined Plane • Forces acting on the object: – The normal (support) force acts perpendicular to the plane – The gravitational force acts straight down • Choose coordinate system with x along the incline and y perpendicular to incline • Replace the force of gravity with its components Acceleration Down Inclined Plane • Newton’s 2nd law: ∑ Fx = mg sin θ = max ∑ Fy = 0 • From 1st equation: a x = g sin θ • Check special cases to see that answer makes sense: θ = 90o θ = 0o Lecture 9 25/26 End of Lecture 9 z Before the next lecture, read Walker Chapter 5, 5.7; Chapter 6, 6.1 - Kinetic Friction z Homework Assignment #5b should be submitted using WebAssign by 11:00 PM on Thursday, Sept. 24. Lecture 9 27/26 What is acceleration in each of these cases? Lecture 9 26/26