dynamics week 1a
TRANSCRIPT
-
8/13/2019 Dynamics Week 1a
1/7
Dynamics MCB 2043
Introduction
September 2013 SemesterDereje Engida Woldemichael (PhD, CEng MIMechE)
Lesson Outcomes At the end of this lecture you should be able to:
Identify classifications of dynamics
-
8/13/2019 Dynamics Week 1a
2/7
Overview Statics vs Dynamics
Mechanics
Basic Concepts
Particles
Rigid bodies
Newtons Laws of motion
Why Dynamics
So Important?
Statics VS.Dynamics
Bodies at RESTor in equilibrium
Bodies in MOTION
Dynamics of
Solid Bodies
Dynamics of
Gasses/Air
Dynamics of
Liquids
e.g. Hydrodynamicse.g. Robotics
e.g. Aerodynamics
-
8/13/2019 Dynamics Week 1a
3/7
-
8/13/2019 Dynamics Week 1a
4/7
Basic Concepts
Particles: - a body of negligible dimensions- a body with dimensions irrelevant to the motion or
the action of forces upon it
A
B
A
BEquivalentParticle
= Rigid Body: - important overall dimensions of the body or changes
in position of the body- negligible deformation (change in shape) of the body
Flexible Body: - deformed body under loads- beyond the scope of this course
Negligible springdeformation
=Rigid body
Newtons Laws of Motion
These are fundamental laws relating forces and motion.
Law I. A particle remains at rest or continues to move in a straight
line with a constant velocity if there is no unbalanced force
acting on it.Sir Isaac Newton
(1643-1727)
Law II. The acceleration of a particle is proportional to the resultant
force acting on it and is in the direction of this force.
F=0 In equilibrium
F=ma Out of equilibrium
Law III. The forces of action and reaction between interacting bodies
are equal in magnitude, opposite in direction, and collinear.
F= F'F F'
Laws Iand IIare strictly true only in an absolute frame of reference (i.e. A particledoes not acceleratefor Law Iand does not rotatefor Law II)
-
8/13/2019 Dynamics Week 1a
5/7
Law II (Most commonly used in dynamics)
F=ma
Where F: resultant force acting on a body (vector)
m: mass of the body (scalar)
a: the resulting acceleration of the body (vector)
F
m
=F=F1+F2+F3+F4+..Fn-1+Fn=ma
F1Fn
F2
F3F4
Fn-1
m
This equation relates applied forces (F) to the motion of a body (a).
Motion can be constrained (forced to follow a specific path: e.g. car trip, train
on tracks)
or unconstrained(can move in any direction: e.g. aircraft flight path, trajectory
of a ball after it is thrown)
Tennis Ball Bouncing
Unconstrained MotionTrain Running on Tracks
Constrained Motion
2-D Coordinate Systems to Describe Motion:
Rectangularcoordinate (x, y)
Polarcoordinate (r,)
Normal(perpendicular) and Tangent(along the path) coordinates
yP
x
r
t
n
-
8/13/2019 Dynamics Week 1a
6/7
An Overview of Mechanics
Statics: The study of
bodies in equilibrium.Dynamics:1. Kinematics concerned with
the geometric aspects of motion
2. Kinetics - concerned with
the forces causing the motion
Mechanics: The study of how bodiesreact to forces acting on them.
Tips for solving dynamics problems1.Read the problem carefully and try to correlate the actual physical
situation with the theory you have studied.
2.Draw any necessary diagrams and tabulate the problem data.
3.Establish a coordinate system and apply the relevant principles,
generally in mathematical form.
4.Solve the necessary equations algebraically as far as practical; then, use a
consistent set of units and complete the solution numerically. Report the
answer with no more significant figures than the accuracy of the given
data.
5.Study the answer using technical judgment and common sense todetermine whether or not it seems reasonable.
6.Once the solution has been completed, review the problem. Try to think
of other ways of obtaining the same solution
-
8/13/2019 Dynamics Week 1a
7/7
Summary Questions1. In dynamics, a particle is assumed to have _________.
A) both translation and rotational motions
B) only a mass
C) a mass but the size and shape cannot be neglected
D) no mass or size or shape, it is just a point
References: R.C. Hibbeler, Engineering Mechanics: Dynamics, SI 13th
Edition, Prentice-Hall, 2012.