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Physics 1D03 - Lecture 19 Kinetic Energy and Work
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Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Mar 28, 2015

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Page 1: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Kinetic Energy and Work

Page 2: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Then the Work-Energy Theorem says:

The total work done by all external forces acting on a particle is equal to the increase in its kinetic energy.

W = ΔK = Kf – Ki

Kinetic Energy

DefinitionDefinition: for a particle moving with speed v, the kinetic energy is

K = ½ mv2 (a SCALAR quantity)

Page 3: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

• Kinetic Energy is measured in joules (1J=1N·m).

• Kinetic energy is a scalar; the work-energy theorem is a scalar relation.

• This theorem is equivalent to Newton’s Second Law. In principle, either method can be used for any problem in particle dynamics.

Page 4: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

How to deal with friction

If there is friction in the system, then:

ΔK=Wf

= -ffd

Since ΔK = Kf - Ki = -ffd

Therefore Kf = Ki - ffd

Page 5: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example 1

A bartender slides a 1-kg glass 3 m along the bar to a customer. The glass is moving at 4 m/s when the bartender lets go, and at 2 m/s when the customer catches it.

a) Find the work done by frictionb) Calculate the force of friction.

Page 6: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example 2

A 6.0 kg block initially at rest is pulled to the right for 3.0m with a force of 12N over a surface.

Determine its final velocity if:

a) the surface has no friction

b) the surface has a coefficient of kinetic friction of 0.15

How else could we solve this problem ???? Try it !!!

Page 7: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Solution

Page 8: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Quiz

a) when you let it go at x=Ab) when it goes through x=0c) when it gets to x=-A, on the other side of x=0d) it always has the same speed

A mass is attached to a horizontal spring and rests on a frictionless table. Starting from the unstretched position at x=0, the spring is displaced by x=A.When does the mass have the highest speed?

Page 9: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example 3

A block of mass 1.6kg resting on a frictionless surface is attached to a horizontal spring with a spring constant k=1.0x103 N/m (for a spring, E= ½ kx2). The spring is compressed to 2.0cm and released from rest.

a) Calculate the speed of the block as it passes the x=0 point.

b) Calculate the block’s speed at the x=1.0 cm point.

c) Calculate the block’s speed the first time is passes though the x=0cm point if there is a constant frictional force of 4.0 N.

Page 10: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Solution

Page 11: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example 4

You drop a rock off the top of the CN Tower (h=553.33m). Use the energy-work theorem to determine the rock’s speed as it hits the ground below.

Page 12: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Quiz

Your friends at the International Space Station (orbiting at 350 km above the Earth’s surface) were tired of you, and pushed you out of an air lock. Assuming negligible initial speed, if the Earth did not have an atmosphere, how fast would you hit the ground:

A) 86 m/s B) 2620 m/sC) 6860 m/sD) depends on the direction you take (straight down, or

at an angle)

Page 13: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

10 min rest

Page 14: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Potential Energy

• Work and potential energy• Conservative and non-conservative forces• Gravitational and elastic potential energy

Page 15: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Gravitational Work

s2 y s1

mg When the block is lowered, gravity does work:

Wg1 = mg.s1 = mgy

or, taking a different route:

Wg2 = mg.s2 = mgy

y

mg

FP = mg

To lift the block to a height y requires work (by FP :)

WP = FPy = mgy

Page 16: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Work done (against gravity) to lift the box is “stored” as

gravitational potential energy Ug:

Ug =(weight) x (height) = mgy (uniform g)

When a block moves up, work done by gravity is negative (decrease speed) When a block moves down, work done by gravity is positive (increase speed)

• The position where Ug = 0 is arbitrary.

• Ug is a function of position only. (It depends only on the relative positions of the earth and the block.)

• The work Wg depends only on the initial and final heights, NOT on the path.

Page 17: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example

• A rock of mass 1kg is released from rest from a 10m tall building. What is its speed as it hits the ground ?

• The same rock is thrown with a velocity of 10m/s at an angle of 45o above the horizontal. What is its speed as it hits the ground.

Page 18: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example

• What minimum speed does a 100g puck need to make it to the top of a 3.0m long 200 frictionless ramp?

Page 19: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Conservative Forces

A force is called “conservative” if the work done (in going from A to B) is the same for all paths from A to B.

An equivalent definition:

For a conservative force, the work done on any closed path is zero.

Total work is zero.

path 1

path 2A

B

W1 = W2

Page 20: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Quiz

a) Yes.b) No.c) Maybe, maybe not.

The diagram at right shows a force which varies with position. Is this a conservative force?

Page 21: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Quiz

a) Yes.b) No.c) Maybe, maybe not.

The diagram at right shows a force which varies with position. Is this a conservative force?

Page 22: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

For every conservative force, we can define a potential energy function U so that

WAB U UA UB

Examples:

Gravity (uniform g) : Ug = mgy, where y is height

Gravity (exact, for two particles, a distance r apart): Ug GMm/r, where M and m are the masses

Ideal spring: Us = ½ kx2, where x is the stretch

Electrostatic forces (we’ll do this in January)

Note the negative

Since: W = ∆K = - ∆U : Kinetic ↔ Potential

Page 23: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Non-conservative forces:• friction• drag forces in fluids (e.g., air resistance)

Friction forces are always opposite to v (the directionof f changes as v changes). Work done to overcome friction is not stored as potential energy, but converted to thermal energy.

Page 24: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

If only conservative forces do work, potential energy is converted into kinetic energy or vice versa, leaving the total constant. Define the mechanical energy E as the sum of kinetic and potential energy:

E K + U = K + Ug + Us + ...

Conservative forces only: W UWork-energy theorem: W K

So, KU 0; which means that E does not change with time:

dE/dt = 0

Conservation of mechanical energy

Page 25: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example: Atwood’s Machine

An Atwood's machine supports masses m1=0.205 kg and m2=0.292 kg. The masses are held at rest beside each other and then released. Once released the 0.292 kg mass accelerates downward.

Neglecting friction, what is the speed of the masses the instant each has moved through 0.424 m?

Page 26: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example: Pendulum

vf

The pendulum is released from rest with the string horizontal.

a) Find the speed at the lowest point (in terms of the length L of the string).

L

Page 27: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example: Pendulum

vf

The pendulum is released from rest at an angle θ to the vertical.

a) Find the speed at the lowest point (in terms of the length L of the string).

θ

Page 28: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

10 min rest

Page 29: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Energy Examples

Page 30: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example

• Tarzan (mass 90kg) swings on a 10m long rope off the top of BSB to save a student (mass 60kg) from falling into a construction hole on campus. If Tarzan starts with the rope in a horizontal position and picks up the student at the bottom of the swing, determine how high they will go.

Page 31: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example

• In a ballistic pendulum a bullet is shot into a block on a string. If the block and bullet swing up by a vertical distance of h, determine the speed of the bullet.

Page 32: Physics 1D03 - Lecture 19 Kinetic Energy and Work.

Physics 1D03 - Lecture 19

Example

• A pendulum of length 1m and mass of 100g is released from an angle 30o. At the bottom of the swing hits a spring of spring constant k=10N/m. Determine the maximum compression of the spring.