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MM203 Mechanics of Machines: Part 2

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1 MM203 Mechanics of Machines: Part 2
Dr. Alan Kennedy

2 Kinetics of systems of particles
Extension of basic principles to general systems of particles Particles with light links Rigid bodies Rigid bodies with flexible links Non-rigid bodies Masses of fluid MM203 Dr. Alan Kennedy

3 Newton’s second law G – centre of mass
Fi – external force, fi – internal force ri – position of mi relative to G MM203 Dr. Alan Kennedy

4 Newton’s second law By definition For particle i
Adding equations for all particles MM203 Dr. Alan Kennedy

5 Newton’s second law Differentiating w.r.t. time gives Also so
(principle of motion of the mass centre) MM203 Dr. Alan Kennedy

6 Newton’s second law Note that is the acceleration of the instantaneous mass centre – which may vary over time if body not rigid. Note that the sum of forces is in the same direction as the acceleration of the mass centre but does not necessarily pass through the mass centre MM203 Dr. Alan Kennedy

7 Example Three people (A, 60 kg, B, 90 kg, and C, 80 kg) are in a boat which glides through the water with negligible resistance with a speed of 1 knot. If the people change position as shown in the second figure, find the position of the boat relative to where it would be if they had not moved. Does the sequence or timing of the change in positions affect the final result? (Answer: x = m). (Problem 4/15, M&K) MM203 Dr. Alan Kennedy

8 Example The 1650 kg car has its mass centre at G. Calculate the normal forces at A and B between the road and the front and rear pairs of wheels under the conditions of maximum acceleration. The mass of the wheels is small compared with the total mass of the car. The coefficient of static friction between the road and the rear driving wheels is 0.8. (Answer: NA = 6.85 kN, NB = 9.34 kN). (Problem 6/5, M&K) MM203 Dr. Alan Kennedy

9 Work-energy Work-energy relationship for mass i is
where (U1-2)i is the work done on mi during a period of motion by the external and internal forces acting on it. Kinetic energy of mass i is MM203 Dr. Alan Kennedy

10 Work-energy For entire system MM203 Dr. Alan Kennedy

11 Work-energy Note that no net work is done by internal forces.
If changes in potential energy possible (gravitational and elastic) then as for single particle MM203 Dr. Alan Kennedy

12 Work-energy For system Now and note that so MM203 Dr. Alan Kennedy

13 Work-energy Since ri is measured from G, Now MM203 Dr. Alan Kennedy

14 Work-energy Therefore
i.e. energy is that of translation of mass-centre and that of translation of particles relative to mass-centre MM203 Dr. Alan Kennedy

15 Example The two small spheres, each of mass m, are rigidly connected by a rod of negligible mass and are released in the position shown and slide down the smooth circular guide in the vertical plane. Determine their common velocity v as they reach the horizontal dashed position. Also find the force R between sphere 1 and the guide the instant before the sphere reaches position A. (Answer: v = 1.137(gr)½, R = 2.29mg). (Problem 4/9, M&K) MM203 Dr. Alan Kennedy

16 Rigid body Motion of particles relative to mass-centre can only be due to rotation of body Velocity of particles due to rotation depends on angular velocity and the distance to centre of rotation. Where is centre of rotation? Need to examine kinematics of rotation MM203 Dr. Alan Kennedy

17 Plane kinematics of rigid bodies
Rigid body distances between points remains unchanged position vectors, as measured relative to coordinate system fixed to body, remain constant Plane motion motion of all points is on parallel planes Plane of motion taken as plane containing mass centre Body treated as thin slab in plane of motion – all points on body projected onto plane MM203 Dr. Alan Kennedy

18 Kinematics of rigid bodies
MM203 Dr. Alan Kennedy

19 Translation All points move in parallel lines or along congruent curves. Motion is completely specified by motion of any point – therefore can be treated as particle Analysis as developed for particle motion MM203 Dr. Alan Kennedy

20 Kinematics of rigid bodies
MM203 Dr. Alan Kennedy

21 Rotation about fixed axis
All particles move in circular paths about axis of rotation All lines on body (in plane of motion) rotate through the same angle in the same time Similar to circular motion of a particle where riO is distance to O, the centre of rotation, and IO is mass moment of inertia about O MM203 Dr. Alan Kennedy

22 Mass moment of inertia Mass moment of inertia in rotation is equivalent to mass in translation Rotation and translation are analogous MM203 Dr. Alan Kennedy

23 General plane motion Combination of translation and rotation
Principles of relative motion used MM203 Dr. Alan Kennedy

24 Rotation Angular positions of two lines on body are measured from any fixed reference direction MM203 Dr. Alan Kennedy

25 Rotation All lines on a rigid body in its plane of motion have the same angular displacement, the same angular velocity, and the same angular acceleration Angular motion does not require the presence of a fixed axis about which the body rotates MM203 Dr. Alan Kennedy

26 Angular motion relations
Angular position, angular velocity, and angular acceleration Similar to relationships between s, v, and a. Also, combining relationships and cancelling out dt MM203 Dr. Alan Kennedy

27 Angular motion relations
If constant angular acceleration Direction of +ve sense must be consistent Analogous to rectilinear motion with constant a Same procedures used in analysis MM203 Dr. Alan Kennedy

28 Example The angular velocity of a gear is controlled according to w = 12 – 3t2 where w, in radians per second, is positive in the clockwise sense and where t is the time in seconds. Find the net angular displacement Dq from the time t = 0 to t = 3 s. Also find the total number of revolutions N through which the gear turns during the 3 seconds. (Answer: Dq = 9 rad, N = 3.66 rev). (Problem 5/5, M&K) MM203 Dr. Alan Kennedy

29 Kinetic energy of rigid body
If rotation about O MM203 Dr. Alan Kennedy

30 Parallel axis theorem Now (P.A.T.) and so MM203 Dr. Alan Kennedy

31 Radius of gyration Radius of gyration
Mass moment of inertia of point mass m at radius of gyration is the same as that for body P.A.T. MM203 Dr. Alan Kennedy

32 Work done on rigid body MM203 Dr. Alan Kennedy

33 Work done by couple Couple is system of forces that causes rotation but no translation Moment about G Moment about O MM203 Dr. Alan Kennedy

34 Work done by couple Moment vector is a free vector
Forces have turning effect or torque Torque is force by perpendicular distance between forces Work done positive or negative MM203 Dr. Alan Kennedy

35 Forces and couples Torque is Also unbalanced force MM203
Dr. Alan Kennedy

36 Work-energy principle
When applied to system of connected bodies only consider forces/moments of system – ignore internal forces/moments. If there is significant friction between components then system must be dismembered MM203 Dr. Alan Kennedy

37 Example A steady 22 N force is applied normal to the handle of the hand-operated grinder. The gear inside the housing with its shaft and attached handle have a combined mass of 1.8 kg and a radius of gyration about their axis of 72 mm. The grinding wheel with its attached shaft and pinion (inside housing) have a combined mass of 0.55 kg and a radius of gyration of 54 mm. If the gear ratio between gear and pinion is 4:1, calculate the speed of the grinding wheel after 6 complete revolutions of the handle starting from rest. (Answer: N = 3320 rev/min). (Problem 6/119, M&K) MM203 Dr. Alan Kennedy

38 Rotation about fixed axis
Motion of point on rigid body MM203 Dr. Alan Kennedy

39 Vector notation Angular velocity vector, w, for body has sense governed by right-hand rule free vector MM203 Dr. Alan Kennedy

40 Vector notation Velocity vector of point A
What are magnitude and direction of this vector? Note that MM203 Dr. Alan Kennedy

41 Vector notation Acceleration of point MM203 Dr. Alan Kennedy

42 Vector notation Vector equivalents
Can be applied in 3D except then angular velocity can change direction and magnitude MM203 Dr. Alan Kennedy

43 Example The T-shaped body rotates about a horizontal axis through O. At the instant represented, its angular velocity is w = 3 rad/s and its angular acceleration is a = 14 rad/s2. Determine the velocity and acceleration of (a) point A and (b) point B. Express your results in terms of components along the n- and t- axes shown. (Answer: vA = 1.2et m/s, aA = −5.6et + 3.6en m/s2, vB = 1.2et + 0.3en m/s, aB = −6.5et + 2.2en m/s2). (Problem 5/2, M&K) MM203 Dr. Alan Kennedy

44 Example The two V-belt pulleys form an integral unit and rotate about the fixed axis at O. At a certain instant, point A on the belt of the smaller pulley has a velocity vA = 1.5 m/s, and the point B on the belt of the larger pulley has an acceleration aB = 45 m/s2 as shown. For this instant determine the magnitude of the acceleration aC of the point C and sketch the vector in your solution. (Answer: aC = m/s2). (Problem 5/16, M&K) MM203 Dr. Alan Kennedy

45 Linear impulse and momentum
Returning to general system: Linear momentum of mass i is For system (assuming m does not change with time) MM203 Dr. Alan Kennedy

46 Linear impulse and momentum
Differentiating w.r.t. time Same as for single particle – only applies if mass constant Same for rigid body MM203 Dr. Alan Kennedy

47 Example The 300 kg and 400 kg mine cars are rolling in opposite directions along a horizontal track with the speeds shown. Upon impact the cars become coupled together. Just prior to impact, a 100 kg boulder leaves the delivery chute and lands in the 300 kg car. Calculate the velocity v of the system after the boulder has come to a rest relative to the car. Would the final velocity be the same if the cars were coupled before the boulder dropped? (Answer: v = m/s). (Problem 4/11, M&K) MM203 Dr. Alan Kennedy

48 Angular impulse and momentum
Considered about a fixed point O and about the mass centre. MM203 Dr. Alan Kennedy

49 Angular impulse and momentum
About O First term is zero since vi × vi =0 so - sum of all external moments (net moment of internal forces is zero) MM203 Dr. Alan Kennedy

50 Angular impulse and momentum
About O: same as for single particle. As before, does not apply if mass is changing. About G MM203 Dr. Alan Kennedy

51 Example The two balls are attached to a light rod which is suspended by a cord from the support above it. If the balls and rod, initially at rest, are struck by a force F = 60 N, calculate the corresponding acceleration aˉ of the mass centre and the rate d2q/dt2 at which the angular velocity of the bar is changing. (Answer: aˉ = 20 m/s2, d2q/dt2 = 336 rad/s2). (Problem 4/17, M&K) MM203 Dr. Alan Kennedy

52 Rigid body Angular momentum Planar motion MM203 Dr. Alan Kennedy

53 Rigid body Angular acceleration MM203 Dr. Alan Kennedy

54 Kinetic diagrams MM203 Dr. Alan Kennedy

55 Kinetic diagrams - translation
Alternative moment equation for rectilinear translation MM203 Dr. Alan Kennedy

56 Kinetic diagrams - translation
Alternative moment equation for curvilinear translation MM203 Dr. Alan Kennedy

57 Example The cart B moves to the right with acceleration a = 2g. If the steady-state angular deflection of the uniform slender rod of mass 3 m is observed to be 20°, determine the value of the torsional spring constant K. The spring, which exerts a moment M = Kq on the rod, is undeformed when the rod is vertical. The values of m and l are 0.5 kg and 0.6 m, respectively. Treat the small end sphere of mass m as a particle. (Answer: K = 46.8 N·m/rad). (Problem 6/16, M&K) MM203 Dr. Alan Kennedy

58 Example The mass of gear A is 20 kg and its centroidal radius of gyration is 150 mm. The mass of gear B is 10 kg and its centroidal radius of gyration is 100 mm. Calculate the angular acceleration of gear B when a torque of 12 N·m is applied to the shaft of gear A. Neglect friction. (Answer: aB = 25.5 rad/s2 (CCW)). (Problem 6/46, M&K) MM203 Dr. Alan Kennedy

59 Example The 28 g bullet has a horizontal velocity of 500 m/s when it strikes the 25 kg compound pendulum, which has a radius of gyration of kO = 925 mm. If the distance h = 1075 mm, calculate the angular velocity w of the pendulum with its embedded bullet immediately after the impact. (Answer: w = rad/s) (Problem 6/174, M&K) MM203 Dr. Alan Kennedy

60 Plane kinematics: absolute motion
Absolute motion analysis Get geometric relationships Get time derivatives to determine velocity and acceleration Straightforward if geometry is straightforward Must be consistent with signs MM203 Dr. Alan Kennedy

61 Example Point A is given a constant acceleration a to the right starting from rest with x essentially 0. Determine the angular velocity w of link AB in terms of x and a. (Problem 5/24, M&K) Answer: MM203 Dr. Alan Kennedy

62 Example The wheel of radius r rolls without slipping, and its centre O has a constant velocity vO to the right. Determine expressions for the velocity v and acceleration of point A on the rim by differentiating its x- and y-coordinates. Represent your result graphically as vectors on your sketch and show that v is the vector sum of two vO vectors. (Problem 5/25, M&K) Answer: MM203 Dr. Alan Kennedy

63 Example One of the most common mechanisms is the slider-crank. Express the angular velocity wAB and the angular acceleration aAB of the connecting rod AB in terms of the crank angle q for a given constant crank speed w0. Take wAB and aAB to be positive counter-clockwise. (Problem 5/54, M&K) Answer: MM203 Dr. Alan Kennedy

64 Plane kinematics: relative velocity
Two points on same rigid body. Motion of one relative to the other must be circular since distance between them is constant. MM203 Dr. Alan Kennedy

65 Plane kinematics: relative velocity
Relative linear velocity is always in direction perpendicular to line joining points MM203 Dr. Alan Kennedy

66 Plane kinematics: relative velocity
MM203 Dr. Alan Kennedy

67 Plane kinematics: relative velocity
Relative velocity principles may also be used in cases where there is constrained sliding contact between two links – A and B may be on different links MM203 Dr. Alan Kennedy

68 Example Determine the angular velocity of the telescoping link AB for the position shown where the driving links have the angular velocities indicated. (Answer: wAB = 0.96 rad/s). (Problem 5/61, M&K) MM203 Dr. Alan Kennedy

69 Example For an interval of its motion the piston rod of the hydraulic cylinder has a velocity VA = 1.2 m/s as shown. At a certain instant q = b = 60°. For this instant determine the angular velocity wBC of the link BC. (Answer: wBC = rad/s). (Problem 5/66, M&K) MM203 Dr. Alan Kennedy

70 Example The mechanism is designed to convert from one rotation to another. Rotation of link BC is controlled by the rotation of the curved slotted arm OA which engages pin P. For the instant represented q = 30° and b, the angle between the tangent to the curve at P and the horizontal, is 40°. If the angular velocity of OA is as shown, determine the velocity of the point C. (Answer: vC = 4.33 m/s). (Problem 5/85, M&K) MM203 Dr. Alan Kennedy

71 Relative acceleration
May need to know velocities first MM203 Dr. Alan Kennedy

72 Example If OA has a CCW angular velocity w0 = 10 rad/s (giving wBC = 5.83 rad/s and wAB = 2.5 rad/s), calculate the angular acceleration of link AB for the position where the coordinates of A are x = −60 mm and y = 80 mm. Link BC is vertical for this position. (Answer: aAB = 2.5 rad/s2). (Problem 5/137, M&K) MM203 Dr. Alan Kennedy

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