Work and energy 1 Work Definition Work done

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Work and energy 1. Work Definition: Work done by forces that oppose the direction

Work and energy 1. Work Definition: Work done by forces that oppose the direction of motion will be negative. Units: [W] = N*m = J Example: A block slides down a rough inclined surface. The forces acting on the block are depicted below. The work done by the frictional force is: A. Positive B. Negative C. Zero Wf = |fk| |Δx| cos(180°) = -|fk| |Δx| < 0 f Work done by the normal force: WN = |N| |Δx| cos(90°) = 0 Work done by weight: Wmg = mg|Δx| cos(θ ) > 0 1

2. Work kinetic energy principle Definition: W=K 2 - K 1 Example: An 80

2. Work kinetic energy principle Definition: W=K 2 - K 1 Example: An 80 -g arrow is fired from a bow whose string exerts an average force of 100 N on the arrow over a distance of 49 cm. What is the speed of the arrow as it leaves the bow? m = 80 g F = 100 N d = 49 cm v 1= 0 v 2 - ? 2

Example: Two blocks (m 1=2 m 2) are pushed by identical forces, each starting

Example: Two blocks (m 1=2 m 2) are pushed by identical forces, each starting at rest at the same start line. Which object has the greater kinetic energy when it reaches the same finish line? 1. Box 1 2. Box 2 3. They both have the same kinetic energy Same force, same distance Same work Same change in kinetic energy Example: A ball is dropped and hits the ground 50 m below. If the initial speed is 0 and we ignore air resistance, what is the speed of the ball as it hits the ground? We can use kinematics or… the WKE theorem Work done by gravity: mgh 3

3. Potential energy a) Gravitational potential energy: b) Elastic potential energy (spring): 8. Conservation

3. Potential energy a) Gravitational potential energy: b) Elastic potential energy (spring): 8. Conservation of energy in mechanics 4

Example: A box of unknown mass and initial speed v 0 = 10 m/s

Example: A box of unknown mass and initial speed v 0 = 10 m/s moves up a frictionless incline. How high does the box go before it begins sliding down? m Only gravity does work (the normal is perpendicular to the motion), so mechanical energy is conserved. We can apply the same thing to any “incline”! Turn-around point: where K=0 E K U v=0 h 5

Example: A roller coaster starts out at the top of a hill of height

Example: A roller coaster starts out at the top of a hill of height h. How fast is it going when it reaches the bottom? h Example: An object of unknown mass is projected with an initial speed, v 0 = 10 m/s at an unknown angle above the horizontal. If air resistance could be neglected, what would be the speed of the object at height, h = 3. 3 m above the starting point? 6

Example: Pendulum (Conservation of energy) Only weight of the pendulum is doing work; weight

Example: Pendulum (Conservation of energy) Only weight of the pendulum is doing work; weight is a conservative force, so mechanical energy is conserved: m θ 0 L The angle on the other side is also θ 0! 7

4. Energy in the simple harmonic motion U E –A A x K t

4. Energy in the simple harmonic motion U E –A A x K t U t E t Total mechanical energy is constant through oscillation: conservation of energy! 8

5. Damped Harmonic Motion x(t) Damping force is proportional to velocity: t b –

5. Damped Harmonic Motion x(t) Damping force is proportional to velocity: t b – damping constant (Shows how fast oscillations decay) Optional math: 9

6. Resonance 10

6. Resonance 10