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Work and Energy Chapter 5 Mrs. Schwartz.

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Presentation on theme: "Work and Energy Chapter 5 Mrs. Schwartz."— Presentation transcript:

1 Work and Energy Chapter 5 Mrs. Schwartz

2 What is work?

3 Work Work is done on an object when a FORCE causes a displacement on an object. W = Fd

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5 Work Work is only done when components of a force are parallel to the objects displacement.

6 W = Fd(cos θ) Work with an angle
If there is a force in a direction that makes an angle, θ, with the direction of the displacement, then W = Fd(cos θ) θ is the angle between the directions of the force and the displacement.

7 Work If θ = 0 (parallel) then Cos0 = 1 Work is done! If θ = 90 (parallel) then Cos90 = 0 No Work done! Work is only done when components of a force are parallel to the objects displacement.

8 Example How much work is done on a vacuum cleaner pulled 3.0m by a force of 50.0N at an angle of 30.0o above the horizontal?

9 Work Force in direction of motion speed increases positive work.
Force opposes motionspeed decreases negative work Force is 90º to motion no work done Object is not in motion no work done

10 Kinetic Energy Kinetic Energy is the energy of an object in motion.
K.E. = ½ mv2 This formula is derived from a motion formula and the work formula. Kinetic energy depends on an object’s mass and velocity.

11 Work-Kinetic Energy Theorem
The net work done on an object is equal to the change in the kinetic energy of the object. Wnet = ΔK.E. = ½ mvf2 - ½ mvi2 = Fnetd

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