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EQUATIONS OF MOTION: GENERAL PLANE MOTION

EQUATIONS OF MOTION: GENERAL PLANE MOTION. Today’s Objectives : Students will be able to: Analyze the planar kinetics of a rigid body undergoing general plane motion. In-Class Activities : • Equations of Motion • Frictional Rolling Problems.

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EQUATIONS OF MOTION: GENERAL PLANE MOTION

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  1. EQUATIONS OF MOTION: GENERAL PLANE MOTION • Today’s Objectives: • Students will be able to: • Analyze the planar kinetics of a rigid body undergoing general plane motion. In-Class Activities: • Equations of Motion • Frictional RollingProblems

  2. The forces shown on the roller’s FBD cause the accelerations shown on the kinetic diagram. = APPLICATIONS As the soil compactor accelerates forward, the front roller experiences general plane motion (both translation and rotation). What are the loads experienced by the roller shaft or bearings?

  3. APPLICATIONS (continued) During an impact, the center of gravity of this crash dummy will decelerate with the vehicle, but also experience another acceleration due to its rotation about point A. How can engineers use this information to determine the forces exerted by the seat belt on a passenger during a crash?

  4. Using an x-y inertial coordinate system, the equations of motions about the center of mass, G, may be written as  Fx = m (aG)x  Fy = m (aG)y  MG = IG a P GENERAL PLANE MOTION (Section 17.5) When a rigid body is subjected to external forces and couple-moments, it can undergo both translational motion as well as rotational motion. This combination is called general plane motion.

  5. P GENERAL PLANE MOTION (continued) Sometimes, it may be convenient to write the moment equation about some point P other than G. Then the equations of motion are written as follows.  Fx = m (aG)x  Fy = m (aG)y  MP =  (Mk)P In this case,  (Mk )P represents the sum of the moments of IGaand maG about point P.

  6. FRICTIONAL ROLLING PROBLEMS When analyzing the rolling motion of wheels, cylinders, or disks, it may not be known if the body rolls without slipping or if it slides as it rolls. For example, consider a disk with mass m and radius r, subjected to a known force P. The equations of motion will be  Fx = m(aG)x => P - F = maG  Fy = m(aG)y => N - mg = 0  MG = IGa => F r = IGa There are4 unknowns (F, N, a, andaG)in these three equations.

  7. FRICTIONAL ROLLING PROBLEMS (continued) Hence, we have to make an assumption to provide another equation. Then we can solve for the unknowns. The 4th equation can be obtained from the slip or non-slip condition of the disk. Case 1: Assume no slipping and use aG =a r as the 4th equation and DO NOT use Ff = sN. After solving, you will need to verify that the assumption was correct by checking if Ff  sN. Case 2: Assume slipping and use Ff = kN as the 4th equation. In this case, aG  ar.

  8. PROCEDURE FOR ANALYSIS Problems involving the kinetics of a rigid body undergoing general plane motion can be solved using the following procedure. 1. Establish the x-y inertial coordinate system. Draw both the free body diagram and kinetic diagram for the body. 2. Specify the direction and sense of the acceleration of the mass center, aG, and the angular acceleration aof the body. If necessary,compute the body’s mass moment of inertia IG. 3. If the moment equation Mp= (Mk)p is used, use the kinetic diagram to help visualize the moments developed by the components m(aG)x, m(aG)y, and IGa. 4. Apply the threeequations of motion.

  9. PROCEDURE FOR ANALYSIS (continued) 5. Identify the unknowns. If necessary (i.e., there are four unknowns), make your slip-no slip assumption (typically no slipping, or the use of aG=ar, is assumed first). 6. Use kinematic equations as necessary to complete the solution. 7. If a slip-no slip assumption was made, check its validity!!! Key points to consider: 1. Be consistent in assumed directions. The direction of aGmust be consistent with a. 2. If Ff = kN is used, Ff must oppose the motion. As a test, assume no friction and observe the resulting motion. This may help visualize the correct direction of Ff.

  10. READING QUIZ 1. If a disk rolls on a rough surface without slipping, the acceleration of the center of gravity (G) will _________ and the friction force will be ______. A) not be equal to a r ; B) be equal to a r ;less thansNequal tokN C) be equal to a r ; less than sN D) None of the above. 2. If a rigid body experiences general plane motion, the sum of the moments of external forces acting on the body about any point P is equal to A) IPa. B) IPa + maP. C) maG. D) IGa +rGP x maP.

  11. EXAMPLE Given: A spool has a mass of 8 kg and a radius of gyration (kG) of 0.35 m. Cords of negligible mass are wrapped around its inner hub and outer rim. There is no slipping. Find: The angular acceleration (a) of the spool. Plan: Focus on the spool. Follow the solution procedure (draw a FBD, etc.) and identify the unknowns.

  12. EXAMPLE (continued) Solution: The moment of inertia of the spool is IG = m (kG)2 = 8 (0.35)2 = 0.980 kg·m 2 Method I Equations of motion: Fy = m (aG)y T+100 -78.48 = 8aG MG = IG a 100 (0.2) – T(0.5) = 0.98 a There are three unknowns, T, aG, a. We need one more equation to solve for 3 unknowns. Since the spool rolls on the cord at point A without slipping, aG= ar. So the third equation is: aG= 0.5a Solving these three equations, we find: a =10.3 rad/s2, aG = 5.16 m/s2, T = 19.8 N

  13. EXAMPLE (continued) Method II Now, instead of using a moment equation about G, a moment equation about A will be used. This approach will eliminate the unknown cord tension (T).  MA=  (Mk)A: 100 (0.7) - 78.48(0.5) = 0.98 a + (8 aG)(0.5) Using the non-slipping condition again yields aG = 0.5a. Solving these two equations, we get a = 10.3 rad/s2, aG = 5.16 m/s2

  14. An 80 kg spool (kG = 0.3 m) is on a rough surface and a cable exerts a 30 N load to the right. The friction force at A acts to the _____ and the aG should be directed to the ______ . • A) right, left B) left, right • C) right, right D) left, left  30N 0.2m • G 0.75m A CONCEPT QUIZ 2. For the situation above, the moment equation about G is: A) 0.75 (FfA) - 0.2(30) = - (80)(0.32) B) -0.2(30) = - (80)(0.32) C) 0.75 (FfA) - 0.2(30) = - (80)(0.32) + 80aG D) None of the above.

  15. GROUP PROBLEM SOLVING Given: A 50 lb wheel has a radius of gyration kG = 0.7 ft. Find: The acceleration of the mass center if M = 35 lb-ft is applied. s = 0.3, k = 0.25. Plan: Follow the problem solving procedure. Solution: The moment of inertia of the wheel about G is IG = m(kG)2 = (50/32.2)(0.7)2 = 0.761 slug·ft2

  16. GROUP PROBLEM SOLVING (continued) FBD: Equations of motion:  Fx = m(aG)x FA = (50/32.2) aG  Fy = m(aG)y NA – 50 = 0  MG = IGa 35 - 1.25 FA= 0.761 a We have 4 unknowns: NA, FA, aG and a. Another equation is needed before solving for the unknowns.

  17. GROUP PROBLEM SOLVING (continued) The three equations we have now are: FA = (50/32.2) aG NA - 50 = 0 35 – (1.25)FA = 0.761 a First, assume the wheel is not slipping. Thus, we can write aG = r a = 1.25 a Now solving the four equations yields: NA = 50.0 lb, FA = 21.3 lb, a = 11.0 rad/s2 , aG= 13.7 ft/s2 The no-slip assumption must be checked. Is FA = 21.3 lb  s NA= 15 lb? No! Therefore, the wheel slips as it rolls.

  18. GROUP PROBLEM SOLVING (continued) Therefore,aG= 1.25a is not a correct assumption. The slip condition must be used. Again, the three equations of motion are: FA = (50/32.2) aG NA – 50 = 0 35 – (1.25)FA = 0.761 a Since the wheel is slipping,the fourth equation is FA = k NA = 0.25NA Solving for the unknowns yields: NA = 50.0 lb FA = 0.25NA = 12.5 lb a = 25.5 rad/s2 aG= 8.05 ft/s2

  19. A 3m 4m 10 N ATTENTION QUIZ 1. A slender 100 kg beam is suspended by a cable. The moment equation about point A is A) 3(10) = 1/12(100)(42)  B) 3(10) = 1/3(100)(42)  C) 3(10) = 1/12(100)(42)  + (100 aGx)(2) D) None of the above. 2. Select the equation that best represents the “no-slip” assumption. A) Ff = s NB) Ff = k N C) aG = r aD) None of the above.

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