Announcements
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Exam #1 breakdown:
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High score: 99%
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Average score: 65% (last year exam #1 → 59%)
Standard deviation 21%
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Note: lowest exam score will be dropped in computing your final grade.
Unit 8: Prelecture Feedback
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Examples similar to homework, rather than reviewing checkpoints
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Need to understand equations in more depth
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...especially springs. Parabola?
Mechanics Lecture 8, Slide 3
Today's Concepts:
Mechanics Lecture 8, Slide 4
Work-Kinetic Energy Theorem
The net work done on a body is equal to the change in kinetic energy of the body
Formal definition of work
(“Force times distance” generalized)
Formal definition of kinetic energy
Mechanics Lecture 8, Slide 5
Work-Kinetic Energy Theorem
If there are several forces acting then W is the work done by the net (total) force:
W
NET
= K
= W
1
+ W
2
+ ...
You can just add up the work done by each force
W
NET
= W
TOT
Mechanics Lecture 8, Slide 6
I move an object from the surface of the Earth to a height of one Earth radius above the Earth, and to a position on the far side of the Earth from the launch position. The object is at rest with respect to the Earth before and after the move.
What is the work that I must do on the object?
If the object were instead moved to “infinity” (or at least very, very far away), what work must I do?
Conservative force: Force with the property that, the work done by the force between r
1
and r
2
is independent of the path taken.
Consequence: The work done by a conservative force around a closed loop = 0.
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Two conservative forces in this course:
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Gravity
Springs
Today's Concepts:
Mechanics Lecture 8, Slide 9
Potential Energy
Can use the properties of conservative forces to store...
“the ability to do work” ≡ “energy”
Example: Store Energy by Raising a Ball
Final position
Initial position
Today's Concepts:
Mechanics Lecture 8, Slide 12
Mechanical Energy
= constant of motion, when only
conservative forces are present
Gravitational potential energy
Kinetic energy
Example
The bob (mass = m ) of a simple pendulum of length L is released from rest at a height H above the equilibrium position.
Compute the tension in the rod when the bob returns to the equilibrium position.
Another Conservative Force: Springs x kx 2
M
Vertical case: zero potential energy in equilibrium position with mass attached
Mechanics Lecture 8, Slide 15
Generalize mechanical energy conservation to conservative systems including springs:
Mechanical Energy
Spring P.E.
K.E.
Gravitational P.E.
Example
A mass M is in contact with a spring (constant k ) which is compressed by an amount x c
from the equilibrium position. After release from rest, the mass detaches from the spring, slides along the frictionless floor and then up the frictionless ramp. What is the height H to which the mass slides before reversing direction?
H
M
Homework Example
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Block slides down frictionless ramp and compresses spring.
How much?
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Apply conservation of mechanical energy.
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Does h block
change after block contacts spring?
Homework Example
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Block slides down frictionless ramp and completes “loop-theloop”. From what minimum height?
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Apply conservation of mechanical energy.
Summary: Potential energy change:
Mechanics Lecture 8, Slide 20