physics lecture 14 instructor: john h. hamilton. last lecture review this week position change in...

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Physics Lecture 14 Instructor: John H. Hamilton

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Lecture overview Kinematic equations for constant acceleration we are going to develop (derive) useful equations for solving constant acceleration problems

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Page 1: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

PhysicsLecture 14

Instructor: John H. Hamilton

Page 2: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

Last Lecture Review

• This week– Position– Change in position wrt time– Change in velocity wrt time

Page 3: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

Lecture overview

• Kinematic equations for constant accelerationwe are going to develop (derive) useful

equations for solving constant acceleration problems

Page 4: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

kinematics

• Branch of classical mechanics that describes the motion of points and objects, and systems of objects, without consideration of the cause of motion

Page 5: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

Constant acceleration

• Kinematic equations – 1) – 2) – 3) – 4) • The o subscript represents values at time zero

Page 6: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

𝑣=𝑣𝑜+𝑎𝑡

Page 7: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

𝑣=𝑣0+𝑣2

Page 8: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

𝑥=𝑥𝑜+𝑣0𝑡+12 𝑎𝑡

2

Page 9: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

𝑣2=𝑣02+2𝑎 (𝑥−𝑥0 )

Page 10: Physics Lecture 14 Instructor: John H. Hamilton. Last Lecture Review This week  Position  Change in position wrt time  Change in velocity wrt time

Lecture Review

• Kinematic equations – 1) – 2) – 3) – 4) • The o subscript represents values at time zero