physics 1d03 - lecture 19 review of scalar product of vectors work by a constant force work by a...

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Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

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Physics 1D03 - Lecture 19  The scalar product or dot product of two vectors gives a scalar result: vector vector = scalar Math Review

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Page 1: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

• Review of scalar product of vectors• Work by a constant force• Work by a varying force• Example: a spring

Work and Energy

Page 2: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Work and EnergyWork and Energy

amF

Energy approach: Net work = increase in kinetic energy

- acceleration at any instant is caused by forces

- equivalent to Newton’s dynamics- scalars, not vectors - compares energies “before and after”

Newton’s approach:

Page 3: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

)ABcos( )A toparallel of (component x )A of (magnitude

BBA

B

A

The scalar product or dot product of two vectors gives a scalar result:

vector • vector = scalar

Math Review

Page 4: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

ScaIar product and cartesian components:

kBjBiBBkAjAiAA

zyx

zyxˆˆˆˆˆˆ

zzyyxx BABABABA

Then,

(note the right-hand-side is a single scalar)

To prove this, expand using the laws of arithmetic (distributive, commutative), and notice that

BA

since, i, j, k are mutually perpendicular

since they are unit vectors1ˆˆˆˆˆˆ0ˆˆˆˆˆˆ

kkjjii

kikjji

and

Page 5: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

MATH QUIZ

A constant force is applied to an object while it undergoes a displacement The work done by is :

N )ˆ3ˆ2ˆ1( kjiF

m. )ˆ2ˆ2ˆ2( kjis F

mN 12 d)J 12 c)

J 12- b)J )ˆ6ˆ4ˆ2( a)

kji

Page 6: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Work

Work by a constant force F during a displacement s:

s

IIF

F

F

Units : N • m = joule (J)

Work = (component of F parallel to motion) x (distance)

We can also write this as:

This is the “scalar product”, or “dot product”. Work is a scalar.

If work is done on a system, W is positive (eg: lifting an object).If work is done by a system, W is negative (eg: object falling)

Work = F • s = Fscos(θ)

Page 7: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Example

(massless pulleys, no friction)

s = 2 m

How much work is done on the rope by Fp?

How much work is done by the upward force on the ball?

100 N

FP

Page 8: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Quiz

The two forces, P and Fg are constant as the block moves up the ramp. The total work done by these two forces combined is:

3 m

2 m

a) 20 Jb) c) 40 J

J 32 J 1030 22

Fg = 5 N

P = 10 N

Page 9: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Quiz

5

4

3

2.5 m

fk = 50 N

w = 100 N

n

Fp = 120

The block is dragged 2.5 m along the slope. Which forces do positive work?

negative work?

zero work?

Page 10: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Quiz

5

4

3

2.5 m

fk = 50 N

w = 100 N

n

Fp = 120

The block is dragged 2.5 m along the slope. Find :a) work done by Fp

b) work done by fk

c) work done by gravityd) work done by normal forcee) Total work on the block

Page 11: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

a) Wp = (120 N)(2.5 m) = 300 J

b) Wf = (- 50 N)(2.5 m) = -125 J

c) Wg =

d) Wn = 0 ( motion)

J 150 m 2.5N) 100(53

Total : 300 + (- 125) + (- 150) = 25 J

mg

IIFmg 53 s

Page 12: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Example: How much work is done to stretch a spring scale from zero to the 20-N mark (a distance of 10 cm)?We can’t just multiply “force times distance” because the force changes during the motion. Our definition of “work” is not complete.

Forces which are not constant:

ix fx

Varying force: split displacement into short segments over which F is nearly constant.

F(x)

x

FFor each small displacement x, the work done is approximately F(x) x, which is the area of the rectangle.

x

Page 13: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Work is the area (A) under a graph of force vs. distance

dxFWx

x

f

i

ix fx

Split displacement into short steps x over which F is nearly constant...

F(x)

xix fx

F(x)

x

Take the limit as x 0 and the number of steps

xFW

We get the total work by adding up the work done in all the small steps. As we let x become small, this becomes the area under the curve, and the sum becomes an integral.

A

Page 14: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

In 1D (motion along the x-axis): dxFWx

x

f

i

Another way to look at it: Suppose W(x) is the total work done in moving a particle to position x. The extra work to move it an additional small distance x is, approximately, W F(x) x.

Rearrange to getx

WxF)(

In the limit as x goes to zero, dx

dWxF )(

Page 15: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Example: An Ideal Spring.

Hooke’s Law: The tension in a spring is proportional to the distance stretched.

or, |F| = k|s|

The spring constant k has units of N/m

Directions: The force exerted by the spring when it is stretched in the +x direction is opposite the direction of the stretch (it is a restoring force): F = -kx

Page 16: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

ix fx

Example: Work by a Spring

Fs

Fskx

Find a function W(x) so thatdx

dWxFs )(

Page 17: Physics 1D03 - Lecture 19 Review of scalar product of vectors Work by a constant force Work by a varying force Example: a spring Work and Energy

Physics 1D03 - Lecture 19

Concept Quiz

A physicist uses a spring cannon to shoot a ball at a stuffed gorilla. The cannon is loaded by compressing the spring 20 cm. The first 10 cm of compression requires work W. The work required for the next 10 cm (to increase the compression from 10 cm to 20 cm) would be

a) Wb) 2Wc) 3Wd) 4W