1. Friction Friction Problem Situations Chapter 5.2 and 5.3

2. Review of Forces Remember to draw your free body diagram F=ma Weight=mg Practice problem: If you lift a stuffed suitcase with a force of 105N, with an acceleration of 0.705 m/s. What is the mass of the suitcase? What is the weight?

3. Your Weight seems different when you accelerate When you are in an elevator how do you feel when you are going up? How about when it is going down? Newton’s Law explains this… You feel the normal force that is pushed up from the floor. This is what weight feels like When the floor exerts a force greater than your weight, you feel heavy. This is called apparent weight.

4. Forces in Springs A compressed or stretched spring exerts a force when it tries to return to its starting place. The amount of stretch in a spring depends on the force you apply. This changes the length of the spring (either compressed or stretched) Use Hooke’s Law to solve these problems Force=spring constant X change in length

5. Spring Constant F=kx K=spring constant N/m The larger the spring constant, the larger the force exerted by the spring. The larger the change in length, the larger the force exerted by the spring. Problem: what is the force required to cause 3.4cm of stretch of a spring with a spring constant of 21 N/m

6. Friction Friction F f is a force that resists motion Friction involves objects in contact with each other. Friction must be overcome before motion occurs. Friction is caused by the uneven surfaces of the touching objects. As surfaces are pressed together, they tend to interlock and offer resistance to being moved over each other.

8. Microscopic Friction Magnified section of a polished steel surface showing surface bumps about 5 x 10 -7 m (500 nm) high, which corresponds to several thousand atomic diameters. Computer graphic from a simulation showing gold atoms (below) adhering to the point of a sharp nickel probe (above) that has been in contact with the gold surface. Surface Roughness Adhesion

9. Friction Frictional forces are always in the direction that is opposite to the direction of motion or to the net force that produces the motion. Friction acts parallel to the surfaces in contact.

10. Types of Friction Static friction: maximum frictional force between stationary objects. Until some maximum value is reached and motion occurs, the frictional force is whatever force is necessary to prevent motion. Static friction will oppose a force until such time as the object “breaks away” from the surface with which it is in contact. The force that is opposed is that component of an applied force that is parallel to the surface of contact.

11. Types of Friction The magnitude of the static friction force F fs has a maximum value which is given by: where μ s is the coefficient of static friction and F N is the magnitude of the normal force on the body from the surface.

12. Types of Friction Sliding or kinetic friction: frictional force between objects that are sliding with respect to one another. Once enough force has been applied to the object to overcome static friction and get the object to move, the friction changes to sliding (or kinetic) friction. Sliding (kinetic) friction is less than static friction. If the component of the applied force on the object (parallel to the surface) exceeds F fs then the magnitude of the opposing force decreases rapidly to a value F k given by: where μ k is the coefficient of kinetic friction.

13. The static frictional force keeps an object from starting to move when a force is applied. The static frictional force has a maximum value, but may take on any value from zero to the maximum, depending on Static Friction what is needed to keep the sum of forces zero.

14. Types of Friction From 0 to the maximum value of the static frictional force F s in the figure, the applied force is resisted by the static frictional force until “breakaway”. Then the sliding (kinetic) frictional force F k is approximately constant.

15. Types of Friction Static and sliding friction are dependent on: The nature of the surfaces in contact. Rough surfaces tend to produce more friction. The normal force (F n ) pressing the surfaces together; the greater F n is, the more friction there is.

16. Types of Friction Rolling friction: involves one object rolling over a surface or another object. Fluid friction: involves the movement of a fluid over an object (air resistance or drag in water) or the addition of a lubricant (oil, grease, etc.) to change sliding or rolling friction to fluid friction.

17. Coefficient of Friction Coefficient of friction (  ): ratio of the frictional force to the normal force pressing the surfaces together.  has no units. Static: Sliding (kinetic):

18. A Model of Friction Friction

19. Static Friction

20. Kinetic Friction

21. The kinetic frictional force is also independent of the relative speed of the surfaces, and of their area of contact. Kinetic Friction and Speed

22. Rolling Friction

23. Horizontal Surface – Constant Speed Constant speed: a = O m/s 2. The normal force pressing the surfaces together is the weight; F n = F w

24. Horizontal Surface: a > O m/s 2

25. If solving for: F x : F f : a:

26. Horizontal Surface: Skidding to a Stop or Slowing Down (a < O m/s 2 ) The frictional force is responsible for the negative acceleration. Generally, there is no F x.

27. Horizontal Surface: Skidding to a Stop or Slowing Down (a < O m/s 2 ) Most common use involves finding acceleration with a velocity equation and finding  k : Acceleration will be negative because the speed is decreasing.

28. Horizontal Surface: Skidding to a Stop or Slowing Down (a < O m/s 2 ) The negative sign for acceleration a is dropped because  k is a ratio of forces that does not depend on direction. Maximum stopping distance occurs when the tire is rotating. When this happens, a = -  s ·g. Otherwise, use a = -  k ·g to find the acceleration, then use a velocity equation to find distance, time, or speed.