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Department of Physics and Astronomy
PHY/EGR Spring 2008 Harry D. Downing Professor and Chair Department of Physics and Astronomy
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Roll Call Fill out Student Information Sheets
Pass out syllabi then go to next slide Take pictures of each student in lab today
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Let’s visit the web for course information.
Downing’s PHY/EGR 321 Home Page physics.sfasu.edu
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Homework Format
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Cover Page Staple at 450 NAME PHY/EGR Date Problems Grade
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Cover Page, Example Pass out some example engineering pad paper
Staple at 450 Harry Downing PHY/EGR Ch 11 – 2, 6, 9, 16 Grade 5, 4, 5, 3 Pass out some example engineering pad paper
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Kinematics of Particles
CHAPTER 11 Kinematics of Particles
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11.1 INTRODUCTION TO DYNAMICS
Galileo and Newton (Galileo’s experiments led to Newton’s laws) Kinematics – study of motion Kinetics – the study of what causes changes in motion Dynamics is composed of kinematics and kinetics
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RECTILINEAR MOTION OF PARTICLES
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11.2 POSITION, VELOCITY, AND ACCELERATION
For linear motion x marks the position of an object. Position units would be m, ft, etc. Average velocity is Velocity units would be in m/s, ft/s, etc. The instantaneous velocity is
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The average acceleration is
The units of acceleration would be m/s2, ft/s2, etc. The instantaneous acceleration is
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Notice If v is a function of x, then One more derivative
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Consider the function Plotted x(m) t(s) v(m/s) t(s) a(m/s2) t(s) 16 32
16 32 t(s) 2 4 6 v(m/s) 12 -12 -24 -36 2 4 6 t(s) a(m/s2) 12 -12 -24 2 4 6 t(s)
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11.3 DETERMINATION OF THE MOTION OF A PARTICLE
Three common classes of motion
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with then get
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or Both can lead to
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Work Some Example Problems
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11.4 UNIFORM RECTILINEAR MOTION
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11.5 UNIFORMLY ACCELERATED RECTILINEAR MOTION
Also
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11.6 MOTION OF SEVERAL PARTICLES
When independent particles move along the same line, independent equations exist for each. Then one should use the same origin and time.
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Relative motion of two particles.
The relative position of B with respect to A The relative velocity of B with respect to A
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The relative acceleration of B with respect to A
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Let’s look at some dependent motions.
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xA G xB C D A B E F Let’s look at the relationships. System has one degree of freedom since only one coordinate can be chosen independently.
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xC xA xB C A B System has 2 degrees of freedom.
Let’s look at the relationships.
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Work Some Example Problems
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11.7 GRAPHICAL SOLUTIONS OF RECTILINEAR-MOTION
Skip this section.
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11.8 OTHER GRAPHICAL METHODS
Skip this section.
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CURVILINEAR MOTION OF PARTICLES
11.9 POSITION VECTOR, VELOCITY, AND ACCELERATION x z y P’ P Let’s find the instantaneous velocity.
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x z y x z y P’ P
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x z y x z y x z y P’ Note that the acceleration is not necessarily along the direction of the velocity. P
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11.10 DERIVATIVES OF VECTOR FUNCTIONS
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Rate of Change of a Vector
The rate of change of a vector is the same with respect to a fixed frame and with respect to a frame in translation.
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11.11 RECTANGULAR COMPONENTS OF VELOCITY AND ACCELERATION
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y x z y P x z
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x z y
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Velocity Components in Projectile Motion
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11.12 MOTION RELATIVE TO A FRAME IN TRANSLATION
x’ z’ y’ B x z y A O
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Work Some Example Problems
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11.13 TANGENTIAL AND NORMAL COMPONENTS
Velocity is tangent to the path of a particle. Acceleration is not necessarily in the same direction. It is often convenient to express the acceleration in terms of components tangent and normal to the path of the particle.
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Plane Motion of a Particle
x y P’ P
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O x y P’ P
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Discuss changing radius of curvature for highway curves
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Motion of a Particle in Space
x y P’ P z The equations are the same.
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11.14 RADIAL AND TRANSVERSE COMPONENTS
Plane Motion x y P
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x y
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Extension to the Motion of a Particle in Space:
Cylindrical Coordinates
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Work Some Example Problems
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