Instantaneous Center of Zero Velocity (IC) (Ani Dönme Merkezi)

Slides:



Advertisements
Similar presentations
PLANE KINETICS OF RIGID BODIES
Advertisements

Kinematics of Rigid Bodies
ROTATION ABOUT A FIXED AXIS
ABSOLUTE MOTION ANALYSIS
Instant Centers of Velocities
Kinematics of Rigid Bodies
Chapter 15 KINEMATICS OF RIGID BODIES
ABSOLUTE MOTION ANALYSIS (Section 16.4)
EQUILIBRIUM OF RIGID BODIES IN TWO DIMENSIONS
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
RIGID BODY MOTION: TRANSLATION & ROTATION
INSTANTANEOUS CENTER (IC) OF ZERO VELOCITY (Section 16.6)
INSTANTANEOUS CENTER OF ZERO VELOCITY Today’s Objectives: Students will be able to: 1.Locate the instantaneous center of zero velocity. 2.Use the instantaneous.
Plane Kinematics of Rigid Bodies
Ch. 16: Rigid Body Kinematics
MENG 372 Chapter 6 Velocity Analysis
Plane Motion of Rigid Bodies: Forces and Accelerations
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
Chapter 11 Angular Momentum.
INSTANTANEOUS CENTER OF ZERO VELOCITY
C O B A w=2 rad/s 2 m a=4 rad/s2 PROBLEMS
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
Kinematics of Rigid Bodies
RELATIVE MOTION ANALYSIS: ACCELERATION
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
ABSOLUTE MOTION ANALYSIS Today’s Objective: Students will be able to: 1.Determine the velocity and acceleration of a rigid body undergoing general plane.
Introduction Instant Centers for a Crank-Slider
ENGR 214 Chapter 15 Kinematics of Rigid Bodies
MOTION RELATIVE TO ROTATING AXES
RELATIVE MOTION ANALYSIS: VELOCITY
PLANAR KINEMATICS OF A RIGID BODY
Lecture 15 – Relative Motion Analysis: Velocity
9 rad/s2 7 rad/s2 13 rad/s2 14 rad/s2 16 rad/s2
DYNAMICS VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Tenth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P.
Dynamics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. Today’s Objectives: Students will be able to:
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
RELATIVE MOTION ANALYSIS: VELOCITY
Today’s Objectives: Students will be able to: a) Resolve the acceleration of a point on a body into components of translation and rotation. b) Determine.
Chapter 11 Angular Momentum. The Vector Product and Torque The torque vector lies in a direction perpendicular to the plane formed by the position vector.
Introduction Sometimes, a body has simultaneously a motion of rotation and translation, such as a wheel of a car, a sphere rolling (not slipping) on the.
Today’s Objectives: Students will be able to: 1.Describe the velocity of a rigid body in terms of translation and rotation components. 2.Perform a relative-motion.
Dynamics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. Today’s Objective: Students will be able to:
Chapter 17 Rigid Body Dynamics. Unconstrained Motion: 3 Equations for x, y, rotation.
DYNAMICS VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Tenth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P.
ABSOLUTE MOTION ANALYSIS Today’s Objective: Students will be able to: 1.Determine the velocity and acceleration of a rigid body undergoing general plane.
EQUILIBRIUM OF RIGID BODIES
Plane Dynamics of Rigid Bodies
VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Seventh Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University CHAPTER.
Dynamics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. Today’s Objectives: Students will be able to:
INSTANTANEOUS CENTER (IC) OF ZERO VELOCITY (Section 16.6)
RELATIVE MOTION ANALYSIS: VELOCITY (Section 16.5)
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
ROTATIONAL MOTION Rotation axis: rotation occurs about an axis that does not move: fixed axis.
RELATIVE MOTION ANALYSIS: VELOCITY
KINEMATICS OF RIGID BODY
Kinematics of Rigid Bodies
INSTANTANEOUS CENTER OF ZERO VELOCITY
ABSOLUTE MOTION ANALYSIS
Kinematics of Rigid Bodies
INSTANTANEOUS CENTER OF ZERO VELOCITY
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
RELATIVE MOTION ANALYSIS: VELOCITY
RELATIVE MOTION ANALYSIS: ACCELERATION
RELATIVE MOTION ANALYSIS: ACCELERATION
RIGID BODY MOTION (Section 16.1)
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
RELATIVE MOTION ANALYSIS: VELOCITY
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
Presentation transcript:

Instantaneous Center of Zero Velocity (IC) (Ani Dönme Merkezi) RIGID BODY KINEMATICS Instantaneous Center of Zero Velocity (IC) (Ani Dönme Merkezi)

In relative velocity analysis, we determined the velocity of a point on a rigid body in plane motion by adding the relative velocity due to rotation about a convenient reference point to the velocity of the reference point. We are now going to solve the problem by choosing a unique reference point which momentarily has zero velocity.

Let’s assume that the body in the figure is in plane motion Let’s assume that the body in the figure is in plane motion. As far as velocities are concerned, the body may be considered to be in pure rotation about an axis, normal to the plane of motion, passing through this point. This axis is called the instantaneous axis of zero velocity and the intersection of this axis with the plane of motion is known as the instantaneous center of zero velocity (point C). For this certain instant, the velocity of point C is zero.

Locating the Instantaneous Center For the body in the figure, let’s assume that the directions of the absolute velocities of any two points A and B on the body are known and are not parallel. If there is a point about which A has absolute circular motion at the instant considered, this point must lie on the normal to through A.

Similar reasoning applies to B, and the intersection of the two perpendiculars will give point C, the instantaneous center of zero velocity. Point C may lie on or off the body. If it lies off the body, it may be visualized as lying on an imaginary extension of the body. The instantaneous center need not be a fixed point in the body or a fixed point in the plane.

If we know the magnitude of the velocity of one of the points, say vA, we may easily obtain the angular velocity of the body and the linear velocity of every point in the body.

Motion of the Instantaneous Center As the body changes its position, the instantaneous center C also changes its position in space and on the body. Although the velocity of the instantaneous center is zero, its acceleration may not be equal to zero. Thus, this point may not be used as an instantaneous center of zero acceleration.

If two or more bodies are connected by pins, the instantaneous center (IC) will be determined separately for each body. In a rotating disk the IC will be the point of contact of the disk with the surface. IC IC for AB IC for BC wBC wAB vB

Absolute IC Point O absolute IC Point O absolute IC Points O1 and O2 absolute IC If the instantaneous center of velocity is fixed for a certain motion of the body, it can be named as “absolute IC”.

Relative IC Point C relative IC Relative IC in infinity For the position shown, rod AB translates, wAB=0 Point P relative IC If the instantaneous center of velocity changes position for a certain motion of the body, it can be named as “relative IC”.

PROBLEMS 1. Determine the angular velocity of link OB if the piston has a velocity of 2 m/s to the right at the instant shown.

PROBLEMS 2. Vertical oscillation of the spring loaded plunger F is controlled by a periodic change in pressure in the vertical hydraulic cylinder E. For the position q = 60°, determine the angular velocity of AD and the velocity of the roller A in its horizontal guide if the plunger F has a downward velocity of 2 m/s.

PROBLEMS 3. The mechanism in the figure is used for riveting. If the velocity of the piston A is vA = 20 m/s for the instant, determine the velocity of D, which moves in the vertical slot.

PROBLEMS 4. The oil pumping unit consists of a walking beam AB, connecting rod BC, and crank CD. If the crank rotates at a constant rate of 6 rad/s (counterclockwise), determine the speed of the rod hanger H at the instant shown. Also find the angular velocities of members BC and AB.

PROBLEMS 5. In relation to the elongation of the hydraulic piston AC, the velocity of point A on the slider is v = 1.25 m/s for the instant when q=tan-1(3/4). At this moment BD is horizontal and DE is vertical. Determine the angular velocities of arms BD and DE and the hydraulic piston AC for this instant. 200 mm