Your SlideShare is downloading. ×
Chapter10 -circular motion
Upcoming SlideShare
Loading in...5
×

Thanks for flagging this SlideShare!

Oops! An error has occurred.

×

Introducing the official SlideShare app

Stunning, full-screen experience for iPhone and Android

Text the download link to your phone

Standard text messaging rates apply

Chapter10 -circular motion

333
views

Published on

Published in: Sports, Technology

0 Comments
1 Like
Statistics
Notes
  • Be the first to comment

No Downloads
Views
Total Views
333
On Slideshare
0
From Embeds
0
Number of Embeds
0
Actions
Shares
0
Downloads
26
Comments
0
Likes
1
Embeds 0
No embeds

Report content
Flagged as inappropriate Flag as inappropriate
Flag as inappropriate

Select your reason for flagging this presentation as inappropriate.

Cancel
No notes for slide

Transcript

  • 1. Chapter 10. Uniform Circular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007
  • 2. Centripetal forces keep these children moving in a circular path.
  • 3. Objectives: After completing this module, you should be able to: • Apply your knowledge of centripetal acceleration and centripetal force to the solution of problems in circular motion. • Define and apply concepts of frequency and period, and relate them to linear speed. • Solve problems involving banking angles, the conical pendulum, and the vertical circle.
  • 4. Uniform Circular Motion Uniform circular motion is motion along a circular path in which there is no change in speed, only a change in direction. Fc v Constant velocity tangent to path. Constant force toward center. Question: Is there an outward force on the ball?
  • 5. Uniform Circular Motion (Cont.) The question of an outward force can be resolved by asking what happens when the string breaks! Ball moves tangent to v path, NOT outward as might be expected. When central force is removed, ball continues in straight line. Centripetal force is needed to change direction.
  • 6. Examples of Centripetal Force You are sitting on the seat next to You are sitting on the seat next to the outside door. What is the the outside door. What is the direction of the resultant force on direction of the resultant force on you as you turn? Is it away from you as you turn? Is it away from center or toward center of the turn? center or toward center of the turn? • Car going around a curve. Fc Force ON you is toward the center.
  • 7. Car Example Continued Reaction Fc F’ The centripetal force is exerted BY the door ON you. (Centrally) There is an outward force, but it does not act There is an outward force, but it does not act ON you. It is the reaction force exerted BY you ON you. It is the reaction force exerted BY you ON the door. It affects only the door. ON the door. It affects only the door.
  • 8. Another Example Disappearing platform at fair. R Fc What exerts the centripetal force in this example and on what does it act? The centripetal force is exerted BY the wall The centripetal force is exerted BY the wall ON the man. A reaction force is exerted by ON the man. A reaction force is exerted by the man on the wall, but that does not the man on the wall, but that does not determine the motion of the man. determine the motion of the man.
  • 9. Spin Cycle on a Washer How is the water removed from clothes during the spin cycle of a washer? Think carefully before answering . . . Does the centripetal force throw water off the clothes? NO. Actually, it is the LACK of a force that NO. Actually, it is the LACK of a force that allows the water to leave the clothes through allows the water to leave the clothes through holes in the circular wall of the rotating holes in the circular wall of the rotating washer. washer.
  • 10. Centripetal Acceleration Consider ball moving at constant speed v in a horizontal circle of radius R at end of string tied to peg on center of table. (Assume zero friction.) n Fc R v W Force Fc and acceleration ac toward center. W =n
  • 11. Deriving Central Acceleration Consider initial velocity at A and final velocity at B: vf vf B R vo A -vo ∆v R s v o
  • 12. Deriving Acceleration (Cont.) Definition: ac = Similar Triangles ac = ∆v t = Centripetal Centripetal acceleration: acceleration: ∆v v = vs = Rt vf ∆v -vo ∆v t R s R s v o mass m vv R 2 v ac = ; R mv Fc = mac = R 2
  • 13. Example 1: A 3-kg rock swings in a circle of radius 5 m. If its constant speed is 8 m/s, what is the centripetal acceleration? 2 v v m m = 3 kg ac = R R R = 5 m; v = 8 m/s 2 (8 m/s) 2 ac = = 12.8 m/s 5m mv Fc = mac = R 2 F = (3 kg)(12.8 m/s2) Fcc = 38.4 N F = 38.4 N
  • 14. Example 2: A skater moves with 15 m/s in a circle of radius 30 m. The ice exerts a central force of 450 N. What is the mass of the skater? Draw and label sketch Fc R mv 2 Fc = ; m= 2 v = 15 m/s R v Fc R 450 N 30 m m=? Speed skater (450 N)(30 m) m= 2 (15 m/s) m = 60.0 kg m = 60.0 kg
  • 15. Example 3. The wall exerts a 600 N force on an 80-kg person moving at 4 m/s on a circular platform. What is the radius of the circular path? Draw and label sketch Newton’s 2nd law for circular motion: m = 80 kg; v = 4 m/s2 Fc = 600 N 2 mv mv F= ; r= r F r=? (80 kg)(4 m/s) r= 600 N 2 rr = 2.13 m = 2.13 m 2
  • 16. Car Negotiating a Flat Turn v Fc R What is the direction of the force ON the car? Ans. Toward Center This central force is exerted BY the road ON the car.
  • 17. Car Negotiating a Flat Turn v Fc R Is there also an outward force acting ON the car? Ans. No, but the car does exert a outward reaction force ON the road.
  • 18. Car Negotiating a Flat Turn m Fc R The centripetal force Fc is that of static friction fs: n Fc = fs fs R v mg The central force FC and the friction force ffss are The central force FC and the friction force are not two different forces that are equal. There is not two different forces that are equal. There is just one force on the car. The nature of this just one force on the car. The nature of this central force is static friction. central force is static friction.
  • 19. Finding the maximum speed for Finding the maximum speed for negotiating a turn without slipping. negotiating a turn without slipping. n fs Fc = fs m v R Fc R mg The car is on the verge of slipping when FC is equal to the maximum force of static friction fs. Fc = fs Fc = mv2 R fs = µsmg
  • 20. Maximum speed without slipping (Cont.) Maximum speed without slipping (Cont.) n Fc = fs fs R R mg m v Fc mv2 v= R = µsmg µsgR Velocity v is maximum Velocity v is maximum speed for no slipping. speed for no slipping.
  • 21. Example 4: A car negotiates a turn of radius 70 m when the coefficient of static friction is 0.7. What is the maximum speed to avoid slipping? m v Fc Fc = R µs = 0.7 mv2 R From which: fs = µsmg v= µsgR g = 9.8 m/s2; R = 70 m v = µ s gR = (0.7)(9.8)(70 m) v = 21.9 m/s v = 21.9 m/s
  • 22. Optimum Banking Angle Fc m v fs w R n θ slow speed By banking a curve at the optimum angle, the normal force n can provide the necessary centripetal force without the need for a friction force. fs = 0 n n w fs θ fast speed w θ optimum
  • 23. Free-body Diagram Acceleration a is toward the center. Set x axis along the direction of ac , i. e., horizontal (left to right). n x mg θ n θ n cos θ θ n n sin θ mg θ mg + ac
  • 24. Optimum Banking Angle (Cont.) n cos θ n n mg θ n sin θ θ Apply Newton’s 2nd Law to x and y axes. mg ΣFx = mac ΣFy = 0 n sin θ = mv2 R n cos θ = mg
  • 25. Optimum Banking Angle (Cont.) n cos θ n n θ n sin θ tan θ = n cos θ n sin θ mg θ mg n sin θ = mv 2 R n cos θ = mg 2 mv 2 R = v tan θ = mg gR 1
  • 26. Optimum Banking Angle (Cont.) n mg θ Optimum Banking Angle θ n cos θ n θ n sin θ mg 2 v tan θ = gR
  • 27. Example 5: A car negotiates a turn of radius 80 m. What is the optimum banking angle for this curve if the speed is to be equal to 12 m/s? n mg n cos θ tan θ = θ θ n n sin θ mg v2 gR = tan θ = 0.184 (12 m/s)2 (9.8 m/s2)(80 m) θ = 10.40 How might you 2 the find mv on the centripetal force FC = car, knowing its mass? R
  • 28. The Conical Pendulum A conical pendulum consists of a mass m revolving in a horizontal circle of radius R at the end of a cord of length L. T cos θ T L θ R T θ h mg T sin θ Note: The inward component of tension T sin θ gives the needed central force.
  • 29. Angle θ and velocity v: T cos θ T L θ θ h mg R Solve two equations to find angle θ T T sin θ = T sin θ mv2 R T cos θ = mg tan θ = v2 gR
  • 30. Example 6: A 2-kg mass swings in a horizontal circle at the end of a cord of length 10 m. What is the constant speed of the mass if the rope makes an angle of 300 with the vertical? θ = 300 T L θ R h 1. Draw & label sketch. 2. Recall formula for pendulum. 2 v tan θ = gR Find: v = ? 3. To use this formula, we need to find R = ? R = L sin 300 = (10 m)(0.5) R=5m
  • 31. Example 6(Cont.): Find v for θ = 300 4. Use given info to find the velocity at 300. R=5m Solve for v=? θ = 300 g = 9.8 m/s2 T v2 tan θ = gR v = gR tan θ 2 h R v = gR tan θ v = (9.8 m/s )(5 m) tan 30 2 L θ R=5m 0 v = 5.32 m/s v = 5.32 m/s
  • 32. Example 7: Now find the tension T in the cord if m = 2 kg, θ = 300, and L = 10 m. T cos θ 2 kg T L θ T= θ h mg R ΣFy = 0: mg = cos θ T T cos θ - mg = 0; (2 kg)(9.8 m/s2) cos 300 T sin θ T cos θ = mg T = 22.6 N T = 22.6 N
  • 33. Example 8: Find the centripetal force Fc for the previous example. θ = 300 2 kg T cos θ L θ h T Fc R T θ mg T sin θ m = 2 kg; v = 5.32 m/s; R = 5 m; T = 22.6 N Fc = mv2 R or Fc = T sin 300 Fcc = 11.3 N F = 11.3 N
  • 34. Swinging Seats at the Fair This problem is identical to the other examples except for finding R. b T L θ d h R=d+b R tan θ = R = L sin θ + b v2 gR and v= gR tan θ
  • 35. Example 9. If b = 5 m and L = 10 m, what will be the speed if the angle θ = 260? v2 tan θ = R=d+b gR L θ b d = (10 m) sin 260 = 4.38 m T d R = 4.38 m + 5 m = 9.38 m R v = gR tan θ v = gR tan θ 2 v = (9.8 m/s )(9.38 m) tan 26 2 0 v = 6.70 m/s v = 6.70 m/s
  • 36. Motion in a Vertical Circle v Consider the forces on a ball attached to a string as it moves in a vertical loop. + v Note also that the positive direction is always along acceleration, i.e., toward the center of the circle. v + v Bottom mg +T T T T mg + mg +mg T v Top of Path Left Side mgTop Top Right Tension is Right no Weight causes Maximum minimum as Weight has no Weight hasT effect T, tensionon W Bottom weight helps small decrease effect on T opposes T inFc forceFc tension Note changes as you click the mouse to show new positions. +
  • 37. v 10 N T + As an exercise, assume that a central force of Fc = 40 N is required to maintain circular motion of a ball and W = 10 N. + R T 10 N v The tension T must The tension T must adjust so that central adjust so that central resultant is 40 N.. resultant is 40 N At top: 10 N + T = 40 N T = _?_N T = 30 Bottom: T – 10 N = 40 N T = __?___ T = 50 N
  • 38. Motion in a Vertical Circle v mg T Resultant force F = mv2 c toward center R R v mg + T = AT TOP: + mg T Consider TOP of circle: T= mv2 R mv2 R - mg
  • 39. Vertical Circle; Mass at bottom v T Resultant force toward center R v mg AT Bottom: T mg + Fc = mv2 R Consider bottom of circle: T - mg = T= mv2 R mv2 R + mg
  • 40. Visual Aid: Assume that the centripetal force required to maintain circular motion is 20 N. Further assume that the weight is 5 N. v R v FC = 20 N at top AND at bottom. mv 2 FC = = 20 N R Resultant central force FC at every point in path! FC = 20 N Weight vector W is downward at every point. W = 5 N, down
  • 41. Visual Aid: The resultant force (20 N) is the vector sum of T and W at ANY point in path. W T T Top: T + W = FC + + v W T + 5 N = 20 N R v FC = 20 N at top AND at bottom. T = 20 N - 5 N = 15 N Bottom: T - W = FC T - 5 N = 20 N T = 20 N + 5 N = 25 N
  • 42. For Motion in Circle v AT TOP: R + T= mg mv2 R T v AT BOTTOM: T mg + T= mv2 R + mg - mg
  • 43. Example 10: A 2-kg rock swings in a vertical circle of radius 8 m. The speed of the rock as it passes its highest point is 10 m/s. What is tension T in rope? 2 v At Top: mg T T= R v mg + T = mv2 mv - mg R R 2 (2 kg)(10 m/s) 2 T= + 2 kg(9.8 m/s ) 8m T = 25 N - 19.6 N T = 5.40 N T = 5.40 N
  • 44. Example 11: A 2-kg rock swings in a vertical circle of radius 8 m. The speed of the rock as it passes its lowest point is 10 m/s. What is tension T in rope? 2 At Bottom: v R T mg T= v T - mg = mv2 mv + mg R R 2 (2 kg)(10 m/s) 2 T= + 2 kg(9.8 m/s ) 8m T = 25 N + 19.6 N T = 44.6 N T = 44.6 N
  • 45. Example 12: What is the critical speed vc at the top, if the 2-kg mass is to continue in a circle of radius 8 m? 0 mv2 v At Top: mg + T = mg R vc occurs when T = 0 R T mv2 vc = gR mg = v R v= gR = (9.8 m/s2)(8 m) vcc= 8.85 m/s v = 8.85 m/s
  • 46. The Loop-the-Loop Same as cord, n replaces T v AT TOP: mg R v AT BOTTOM: n mg + + n= mv2 R n mv2 n= + mg R - mg
  • 47. The Ferris Wheel v AT TOP: n R v + mg AT BOTTOM: n mg + n mg - n= n = mg - mv2 = + mg R mv2 R mv2 R
  • 48. Example 13: What is the apparent weight of a 60-kg person as she moves through the highest point when R = 45 m and the speed at that point is 6 m/s? n mg Apparent weight will be the normal force at the top: mv2 mg - n = n = mg R (60 kg)(6 m/s) 2 2 n = 60 kg(9.8 m/s ) − 45 m + v R v - mv2 R n = 540 N n = 540 N
  • 49. Summary Centripetal Centripetal acceleration: acceleration: v= µsgR Conical pendulum: 2 v ac = ; R mv Fc = mac = R v2 tan θ = gR v= gR tan θ 2
  • 50. Summary: Motion in Circle v AT TOP: mg R v AT BOTTOM: T mg + + mv2 - mg T= R T mv2 + mg T= R
  • 51. Summary: Ferris Wheel v AT TOP: n R v + mg AT BOTTOM: n mg + n mg - n= n = mg - mv2 = + mg R mv2 R mv2 R
  • 52. CONCLUSION: Chapter 10 Uniform Circular Motion