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PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165 Dr. Derrick Boucher Assoc. Prof. of Physics Session 3-4, Chapter 4
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PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Jan 19, 2016

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PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165. Dr. Derrick Boucher Assoc. Prof. of Physics. Session 3-4, Chapter 4. Chapter 4. Simple Projectile Motion Circular motion Centripetal Acceleration in Uniform Circular Motion Rotational/Translational comparisons. - PowerPoint PPT Presentation
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Page 1: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

PHY 2048CGeneral Physics I with lab

Spring 2011CRNs 11154, 11161 & 11165

Dr. Derrick BoucherAssoc. Prof. of Physics

Session 3-4, Chapter 4

Page 2: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Chapter 4

• Simple Projectile Motion

•Circular motion

•Centripetal Acceleration in Uniform

Circular Motion

•Rotational/Translational comparisons

Page 3: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Chapter 4 Practice Problems

Chap 4: 7, 37, 47, 49, 61, 65

Unless otherwise indicated, all practice material is from the “Exercises and Problems” section at the end of the chapter. (Not “Questions.”)

Page 4: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

2-D Kinematics

•The x and y components of the motion are treated

separately.

•Do not mix up x and y data when setting up and

solving equations.

•Good strategy: separate paper into “X” and “Y”

columns.

•Certain events can connect x and y motion at

particular moments (certain t values).

Page 5: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

2-D Kinematics EquationsGeneral 2-D motion

“Projectile” motionay = -g, ax = 0

Page 6: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Example problem Chapter 4 #10 (p. 120)

Page 7: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Circular Motion•Radius is constant (or unimportant)•“Position” is an angle, in radians, θ•Velocity is radians per second, ω (that’s “omega”, not “curly double-u.”)•Acceleration can be along the tangent to the circle, at , or in a radial or “centripetal” direction, ac .

2rad/sin with rat

Page 8: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

s

θ

Page 9: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Example problem Chapter 4 #38 (p. 122)

Page 10: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Centripetal Acceleration

Page 11: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165
Page 12: PHY 2048C General Physics I with lab Spring 2011 CRNs 11154, 11161 & 11165

Example problem Chapter 4 #62 (p. 123)