1 Chapter 5 Applying Newton s Laws PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun
2 Goals for Chapter 5 To use and apply Newton s Laws Connect these laws to Kinematics To study friction and fluid resistance To consider forces in circular motion First in Equilibrium (Newton s First Law) Then, in non-equilibrium (Second Law)
3 Using Newton s First Law when forces are in equilibrium
4 Netwon s laws problems 1. Draw the free body diagram (only forces ON the object, not the ones exerted by the object) 2. Decompose the forces along X and Y directions 3. Write down Newton s 2 nd laws for each direction and each object 4. If more than one object determine their relation (tension forces, acceleration, etc.)
5 1-D equilibrium Consider an athlete hanging on a massless rope.
6 Figure 5.3 PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun
7 A crate on an inclined plane An object on an inclined plane will have components of force in x and y space.
8 Person in an elevator Moving in an arbitrary direction
9 Connected - Two bodies with same acceleration magnitude Draw the two-free body diagrams. The tension from the mass hanging is the same force that draws the cart up the ramp.
10 Box on an inclined plane A box with mass m is placed on a frictionless incline with angle q and is allowed to slide down. a) What is the normal force? b) What is the acceleration of the box? c) How long does it take to fall if the ramp has a length L? F N q mg cosq q mg sinq w B =mg x : mgsinq = ma x y : F N - mgcosq = 0 a x = gsinq
11 Watch for this common error A good road sign is to be sure that the normal force comes out perpendicular to the surface.
12 Friction Two types of friction: 1. Kinetic: The friction force that slows things down 2. Static: The force that makes it hard to even get things moving
13 Refrigerator If you push a refrigerator when there is no friction what happens? In the real world what happens? Especially when it s fully loaded and on a sticky kitchen floor? When does static friction kick in? When does kinetic friction kick in?
14 Frictional forces, kinetic and static Figures 5.17 and 5.18 Friction can keep an object from moving or slow its motion from what we last calculated on an ideal, frictionless surface. Microscopic imperfections cause nonideal motion.
15 Applied force is proportional until the object moves Figure 5.19 Notice the transition between static and kinetic friction. F f-s <μ s F N Ff-k=μkFN If you use the maximum static friction in all cases, there is a big problem!
16 Static Friction This is more complicated For static friction, the friction force can vary F Friction µ Static F Normal Example of the refrigerator: If I don t push, what is the static friction force? What if I push a little?
17 Kinetic Friction For kinetic friction, it turns out that the larger the Normal Force the larger the friction. We can write F Friction = µ Kinetic F Normal Warning: Here µ is a constant THIS IS NOT A VECTOR EQUATION!
18 Notice the effect of friction in horizontal motion Moving a 500 N crate has two parts: getting the motion to begin and then the effect of friction on constant velocity motion.
19 Pulling Against Friction A box of mass m is on a surface with coefficient of kinetic friction mu. You pull with constant force F P at angle Q. The box does not leave the surface and moves to the right. 1. What is the acceleration? 2. What angle maximizes the acceleration? Q Þ x : x : F P cosq - µ K F N = ma x y : F N + F P sinq - mg = 0 F N = mg - F P sinq F P cosq - µ K (mg - F P sinq) = ma x a x = F P m cosq - µ Kg + µ K F P m sinq d(a x ) = - F P dq q max m sinq + µ K F P m cosq = 0 Þ q max = tan -1 µ K
20 Is it better to push or pull a sled? You can pull or push a sled with the same force magnitude, F P, but different angles Q, as shown in the figures. Assuming the sled doesn t leave the ground and has a constant coefficient of friction, m, which is better? F P
21 Box on an inclined plane 2 Same problem as before, but now friction is not negligible and the coefficient of friction is µ. The inclined plane is adjustable and we change q from 0 to 90 degrees. Mass is known and is equal to m. Calculate and draw a graph of: Friction force as a function of q Acceleration of the box as a function of q F f <μf N mg cosq q F N w B =mg If q>q max q x : mgsinq - µ K F N = ma x If static x : mgsinq - F f = 0 y : F N - mgcosq = 0 mg sinq Þ F f = mgsinq µ s F N = mgsinq max µ s mgcosq max = mgsinq max tanq max = µ s y : F N - mgcosq = 0 Þ mgsinq - µ k mgcosq = ma x
26 The dynamics of uniform circular motion In uniform circular motion, both the acceleration and force are centripetal. When going in a circle the choice of coordinates is NOT optional. One of the axis has to point towards the center and in this case å F = ma r c = m v2 R
27 Netwon s laws problems 1. Draw the free body diagram (only forces ON the object, not the ones exerted by the object) 2. Choose coordinates (chose one along the direction of motion if going straight) for each object. Choose + in the direction of motion. IF there is circular motion ONE of the axis has to point towards the center (+ towards center). Decompose the forces that are not along the coordinates 3. Write down Newton s 2 nd laws for each direction and each object. For the one going around a circle the acceleration is a c =v 2 /R. 4. If more than one object determine their relation (force, acceleration, etc.)
28 Examining a misnomer People have adopted the pop-culture use of centrifugal force but it really results from reference frames. It is fictional and results from a car turning while a person continues in straight-line motion (for example).
29 Hanging ball going on circles For the situation below, if only L and the angle are known, (a) What is the tension in the cord? (b) What is the time it takes the ball to go around once? å F r = F T sin b = m 2 v R = m 2 v Lsin b å F y = F T cos b - mg = 0 F T = mg cosb Þ mg cosb sin b = m 4p 2 Lsin b T 2 T = 2p L cos b g
30 Rounding unbanked curve: maximum speed Given a coefficient of static friction, μ s, what is the maximum speed the car can go around the curve without skidding? å F r = F f = m v2 R åf y = F N - mg = 0 F f -max = µ s F N Þ µ s F N = m v 2 max R Þ v max = µ s gr
31 Rounding banked curve: maximum speed What is the angle you need to go around the curve at speed v without friction? å F r = F N sinb = m v2 R åf r = F N cosb - mg = 0 F N = mg cosb Þ mg v2 sin b = mgtanb = m cosb R Þ v = gr tanb
32 Circular and linear motion (2 Objects) The table is frictionless. What must the velocity be for the hanging mass M (2 kg) to remain stationary? Radius is 20 cm. The small mass m is 1 kg.
33 Q5.11 A sled moves on essentially frictionless ice. It is attached by a rope to a vertical post set in the ice. Once given a push, the sled moves around the post at constant speed in a circle of radius R. If the rope breaks, A. the sled will keep moving in a circle. B. the sled will move on a curved path, but not a circle. C. the sled will follow a curved path for a while, then move in a straight line. D. the sled will move in a straight line.
34 Q5.12 A pendulum bob of mass m is attached to the ceiling by a thin wire of length L. The bob moves at constant speed in a horizontal circle of radius R, with the wire making a constant angle with the vertical. The tension in the wire A. is greater than mg. B. is equal to mg. C. is less than mg. D. could be two of the above, depending on the values of m, L, R, and. E. could be all three of the above, depending on the values of m, L, R, and.
35 Hanging balls What is the tension on each string and the force that the balls exert on each other? The mass of each mass is 15 kg and the diameter 25 cm. This example was worked out in class 25 cm Try to do an example with different masses, e.g., one is 10 Kg and the other 20 Kg.
36 Q5.12 A pendulum bob of mass m is attached to the ceiling by a thin wire of length L. The bob moves at constant speed in a horizontal circle of radius R, with the wire making a constant angle b with the vertical. The tension in the wire A. is greater than mg. B. is equal to mg. C. is less than mg. D. is any of the above, depending on the bob s speed v.
37 Q5.13 A pendulum of length L with a bob of mass m swings back and forth. At the low point of its motion (point Q ), the tension in the string is (3/2)mg. What is the speed of the bob at this point? A. 2 gl B. 2gL C. gl P R D. gl 2 Q E. gl 2
38 Forces Assume no friction. Which way will it move? a) Left b) Right c) Stays balanced and will not move
39 Q5.5 A lightweight crate (A) and a heavy crate (B) are side by side on a frictionless horizontal surface. You are applying a horizontal force F to crate A. Which of the following forces should be included in a free-body diagram for crate B? A. the weight of crate B B. the force of crate B on crate A C. the force F that you exert F A B D. the acceleration of crate B E. more than one of the above
40 Q5.6 A toboggan of weight w (including the passengers) slides down a hill of angle a at a constant speed. Which statement about the normal force on the toboggan (magnitude n) is correct? A. n = w B. n > w C. n < w D. not enough information given to decide
41 Q5.9 Blocks A and C are connected by a string as shown. When released, block A accelerates to the right and block C accelerates downward. There is friction between blocks A and B, but not enough to prevent block B from slipping. If you stood next to the table during the time that block B is slipping on top of block A, you would see A. block B accelerating to the right. B. block B accelerating to the left. C. block B moving at constant speed to the right. D. block B moving at constant speed to the left.
42 A more complicated pulley problem Here there is no friction. What is the acceleration of each mass? - F N T T T - m 1 g + m 2 g x : å F x = T = m 1 a 1 y : å F y = F N - m 1 g = 0 + x : 0 = 0 y : å F y = m 2 g - 2T = m 2 a 2 The next key thing to notice is that a 1 is twice a 2 : this is because the length of the cord is conserved and if object 1 moves 1 meter to the left then object 2 moves 1/2 a meter down. Then: T = m 1 a 1 m 2 g - 2T = m 2 a 1 2 a Þ m 2 g - 2m 1 a 1 = m m Þ a 1 = 2 g and a 2m 1 + (m 2 /2) 2 = m 2 g 4m 1 + m 2
Chapter 5 Applying Newton s Laws PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by James Pazun Copyright 2008 Pearson Education Inc., publishing
Chapter 5 Applying Newton s Laws PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Copyright 2012 Pearson Education Inc. To use
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