VECTOR MECHANICS FOR ENGINEERS: CHAPTER DYNAMICS
Tenth Edition
CHAPTER VECTOR MECHANICS FOR ENGINEERS:
18 DYNAMICS Ferdinand P. Beer
E. Russell Johnston, Jr. Phillip J. Cornwell Lecture Notes: Brian P. Self
California Polytechnic State University
KKiinnetmicas toicf sRiogfidRBigoiddies in BoTdhiereseinDiTmherneseions Dimensions
? 2013 The McGraw-Hill Companies, Inc. All rights reserved.
Tenth Edition
Vector Mechanics for Engineers: Dynamics
Contents
Introduction
Rigid Body Angular Momentum in Three Dimensions
Principle of Impulse and Momentum
Kinetic Energy
Sample Problem 18.1
Sample Problem 18.2
Motion of a Rigid Body in Three Dimensions Euler's Equations of Motion and D'Alembert's Principle
Motion About a Fixed Point or a Fixed Axis
Sample Problem 18.3
Motion of a Gyroscope. Eulerian Angles
Steady Precession of a Gyroscope
Motion of an Axisymmetrical Body Under No Force
? 2013 The McGraw-Hill Companies, Inc. All rights reserved.
18 - 2
Tenth Edition
Vector Mechanics for Engineers: Dynamics
Three dimensional analyses are needed to determine the forces and moments on the gimbals of gyroscopes, the rotors of amusement park rides, and the housings of wind turbines.
? 2013 The McGraw-Hill Companies, Inc. All rights reserved.
18 - 3
Tenth Edition
Vector Mechanics for Engineers: Dynamics
Introduction
? The fundamental relations developed for
the plane motion of rigid bodies may also
be applied to the general motion of three
dimensional bodies.
? The relation
HG
I
which was used
to determine the angular momentum of a
rigid slab is not valid for general three
dimensional bodies and motion.
F ma
MG
H G
? The current chapter is concerned with evaluation of the angular momentum and its rate of change for three dimensional motion and application to effective forces, the impulse-momentum and the work-energy principles.
? 2013 The McGraw-Hill Companies, Inc. All rights reserved.
18 - 4
Tenth Edition
Vector Mechanics for Engineers: Dynamics
Rigid Body Angular Momentum in Three Dimensions
? Angular momentum of a body about its mass center,
HG
n
ri
vi
mi
n
ri
rimi
i1
i1
? The x component of the angular momentum,
Hx
n
yi riz
zi riy
mi
i1
n
yi x yi y xi zi z xi x zi mi
i1
n
x
yi2 zi2
mi
n
y xi yimi
n
z zi ximi
i1
i1
i1
H x x y2 z2 dm y xy dm z zx dm
I x x I xy y I xz z
H y I yx x I y y I yz z
H z I zx x I zy y I z z
? 2013 The McGraw-Hill Companies, Inc. All rights reserved.
18 - 5
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