Presentation on theme: "Chapter 15 KINEMATICS OF RIGID BODIES"— Presentation transcript:
1 Chapter 15 KINEMATICS OF RIGID BODIES zIn rigid body translation, all points of the body have the same velocity and the same acceleration at any given instant.A’BqPfConsidering the rotation of a rigid body about a fixed axis, the position of the body is defined by the angle q that the line BP, drawn from the axis of rotation to a point P of the body,rOxyAforms with a fixed plane. The magnitude of the velocity of P is.dsdtv = = rq sin f.where q is the time derivative of q.Sharif University-Aerospace Dep. Fall 2004
2 . ds v = = rq sin f dt dr v = = w x r dt . w = wk = qk z A’The velocity of P is expressed asBqdrdtPfv = = w x rrOxwhere the vectoryA.w = wk = qkis directed along the fixed axis of rotation and represents the angular velocity of the body.
3 . dr v = = w x r dt w = wk = qk a = a x r + w x (w x r) .. . zdrdt.A’v = = w x rw = wk = qkBDenoting by a the derivative dw/dt of the angular velocity, we express the acceleration of P asqPfrOxa = a x r + w x (w x r)yAdifferentiating w and recalling that k is constant in magnitude and direction, we find that...a = ak = wk = qkThe vector a represents the angular acceleration of the body and is directed along the fixed axis of rotation.
4 v = wk x r at = ak x r at = ra an= -w2 r an = rw2 y Consider the motion of a representative slab located in a plane perpendicualr to the axis of rotation of the body. The angular velocity is perpendicular to the slab, so the velocity of point P of the slab isv = wk x rPOrxw = wkv = wk x rwhere v is contained in the plane of the slab. The acceleration of point P can be resolved into tangential and normal components respectively equal toyat = ak x rPan= -w2 rOxw = wkat = ak x r at = raa = akan= -w2 r an = rw2
5 dq w = dt dw d2q a = = dt dt2 dw w = a dq The angular velocity and angular acceleration of the slab can be expressed asdqdtw =dwdtd2qdt2a = =ordwdqw = aTwo particular cases of rotation are frequently encountered: uniform rotation and uniformly accelerated rotation. Problems involving either of these motions can be solved by using equations similar to those for uniform rectilinear motion and uniformly accelerated rectilinear motion of a particle, where x, v, and a are replaced by q, w, and a.
6 vB = vA + vB/A vA vA wk vB vA vB/A y’wkvB(fixed)vAx’AAArB/AvB/ABBBPlane motion = Translation with A Rotation about AThe most general plane motion of a rigid slab can be considered as the sum of a translation and a rotation. The slab shown can be assumed to translate with point A, while simultaneously rotating about A. It follows that the velocity of any point B of the slab can be expressed asvB = vA + vB/Awhere vA is the velocity of A and vB/A is the relative velocity of B with respect to A.
7 vB/A = wk x rB/A vB/A = (rB/A )w = rw vAvAvB/Ay’wkvB(fixed)vAx’vAvBAAArB/AvB/ABBBPlane motion = Translation with A Rotation about AvB = vA + vB/ADenoting by rB/A the position of B relative to A, we note thatvB/A = wk x rB/A vB/A = (rB/A )w = rwThe fundamental equation relating the absolute velocities of points A and B and the relative velocity of B with respect to A can be expressed in the form of a vector diagram and used to solve problems involving the motion of various types of mechanisms.
8 Another approach to the solution of problems involving the velocities of the points of a rigid slab in plane motion is based on determination of the instantaneous center of rotation C of the slab.CCvBBvBAvAvA
9 aB = aA + aB/A aA aA aB/A aB (aB/A)n aA (aB/A)t y’aAwkaAakaB/AaBx’AAA(aB/A)naA(aB/A)tBBBPlane motion = Translation with A Rotation about AThe fact that any plane motion of a rigid slab can be considered the sum of a translation of the slab with reference to point A and a rotation about A is used to relate the absolute accelerations of any two points A and B of the slab and the relative acceleration of B with respect to A.aB = aA + aB/Awhere aB/A consists of a normal component (aB/A )n of magnitude rw2 directed toward A, and a tangential component (aB/A )t of magnitude ra perpendicular to the line AB.
10 aB = aA + aB/A aA aA aB/A aB (aB/A)t (aB/A)n aA y’aAwkaAakaB/AaBx’AAA(aB/A)t(aB/A)naABBBPlane motion = Translation with A Rotation about AaB = aA + aB/AThe fundamental equation relating the absolute accelerations of points A and B and the relative acceleration of B with respect to A can be expressed in the form of a vector diagram and used to determine the accelerations of given points of various mechanisms.(aB/A)n(aB/A)taAaBaB/A
11 aB = aA + aB/A aA aA aB/A aB (aB/A)t (aB/A)n aA y’aAwkaAakaB/AaBx’AAA(aB/A)t(aB/A)naABBBPlane motion = Translation with A Rotation about AaB = aA + aB/A(aB/A)n(aB/A)taAaBaB/AThe instantaneous center of rotation C cannot be used for the determination of accelerations, since point C , in general, does not have zero acceleration.
12 . . (Q)OXYZ = (Q)Oxyz + W x Q Y The rate of change of a vector is the same with respect to a fixed frame of reference and with respect to a frame in translation. The rate of change of a vector with respect to a rotating frame of reference is different. The rate of change of a generalyQAjxiWOXkvector Q with respect a fixed frame OXYZ and with respect to a frame Oxyz rotating with an angular velocity W isZz..(Q)OXYZ = (Q)Oxyz + W x QThe first part represents the rate of change of Q with respect to the rotating frame Oxyz and the second part, W x Q, is induced by the rotation of the frame Oxyz.
13 vP = vP’ + vP/F . Y vP/F = (r)Oxy Consider the two-dimensional analysis of a particle P moving with respect to a frame F rotating with an angular velocity W about a fixed axis. The absolute velocity of P can be expressed asvP’ = W x rPP’yrxOXWvP = vP’ + vP/Fwhere vP = absolute velocity of particle PvP’ = velocity of point P’ of moving frame F coincidingwith PvP/F = velocity of P relative to moving frame FThe same expression for vP is obtained if the frame is in translation rather than rotation.
14 aP = aP’ + aP/F + ac . . Y vP/F = (r)Oxy When the frame is in rotation, the expression for the acceleration of P contains an additional term ac called the complementary acceleration or Coriolis acceleration.vP’ = W x rPP’yrxOXWaP = aP’ + aP/F + acwhere aP = absolute acceleration of particle PaP’ = acceleration of point P’ of moving frame Fcoinciding with PaP/F = acceleration of P relative to moving frame F.ac = 2W x (r)Oxy = 2W x vP/F= complementary, or Coriolis, acceleration
15 aP = aP’ + aP/F + ac . . Y vP/F = (r)Oxy vP’ = W x r aP = absolute acceleration ofparticle PPP’yaP’ = acceleration of point P’ ofmoving frame F coincidingwith PrxOXaP/F = acceleration of P relative tomoving frame FW.ac = 2W x (r)Oxy = 2W x vP/FSince W and vP/F are perpendicular to each other in the case of plane motion, the Coriolis acceleration has a magnitudeac = 2WvP/F . Its direction is obtained by rotating the vector vP/F through 90o in the sense of rotation of the moving frame. The Coriolis acceleration can be used to analyze the motion of mechanisms which contain parts sliding on each other.
16 dr v = = w x r dt a = a x r + w x (w x r) w a In three dimensions, the most general displacement of a rigid body with a fixed point O is equivalent to a rotation of the body about an axis through O. The angular velocity w and the instantaneous axis of rotation of the body at a givenPrOinstant can be defined. The velocity of a point P of the body can be expressed asdrdtv = = w x rDifferentiating this expression, the acceleration isa = a x r + w x (w x r)Since the direction of w changes from instant to instant, the angular acceleration a is, in general, not directed along the instanteneous axis of rotation.
17 aB = aA + a x rB/A + w x (w x rB/A) Y’The most general motion of a rigid body in space is equivalent, at any given instant, to the sum of a translation and a rotation. Considering two particles A and B of the bodyawBYrB/AAZ’X’vB = vA + vB/ArAOwhere vB/A is the velocity of B relative to a frame AX’Y’Z’ attached to A and of fixed orientation. Denoting by rB/AXZthe position vector of B relative to A, we writevB = vA + w x rB/Awhere w is the angular velocity of the body at the instant considered. The acceleration of B is, by similar reasoningaB = aA + aB/AaB = aA + a x rB/A + w x (w x rB/A)or
18 XYZxyzOijkPWArConsider the three-dimensional motion of a particle P relative to a frame Oxyz rotating with an angular velocity W with respect to fixed frame OXYZ. The absolute velocity vP of P can be expressed asvP = vP’ + vP/Fwhere vP = absolute velocity of particle PvP’ = velocity of point P’ of moving frame F coincidingwith PvP/F = velocity of P relative to moving frame F
19 YyPThe absolute acceleration aP of P is expressed asArjxiWaP = aP’ + aP/F + acOXkwhere aP = absolute acceleration of particle PZaP’ = acceleration of point P’ of movingframe F coinciding with PzaP/F = acceleration of P relative to movingframe F.ac = 2W x (r)Oxy = 2W x vP/F= complementary (Coriolis) accelerationThe magnitude ac of the Coriolis acceleration is not equal to 2WvP/F except in the special case when W and vP/F are perpendicular to each other.
20 vP = vP’ + vP/F aP = aP’ + aP/F + ac Y’ The equations y P rP/A x and A Z’rPremain valid when the frame Axyz moves in a known, but arbitrary, fashion with respect to the fixed frame OXYZ, provided that therAzOXZmotion of A is included in the terms vP’ and aP’ representing the absolute velocity and acceleration of the coinciding point P’.Rotating frames of reference are particularly useful in the study of the three-dimensional motion of rigid bodies.
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