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Equipment. Clear Tape. Mr. Klapholz Shaker Heights High School. Forces and Fields (6). In the most fundamental equations about the universe, we find fields . Black holes, the Aurora Borealis, and microwave ovens all are understood in terms of fields. Fields are abstract, but quite real. - PowerPoint PPT Presentation
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Equipment • Clear Tape
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Page 1: Equipment

Equipment

• Clear Tape

Page 2: Equipment

Forces and Fields (6)

In the most fundamental equations about the universe, we find fields.

Black holes, the Aurora Borealis, and microwave ovens all are understood in terms of fields.

Fields are abstract, but quite real.

Mr. KlapholzShaker Heights

High School

Page 3: Equipment

Electricity

Page 4: Equipment

Fun with clear tape that you can try at home

• Make two pieces of tape have the same type of charge

• See what like charges do.• See what an uncharged object does to a

charged object.• Make two pieces with unlike charge.• See what unlike charges do.

Page 5: Equipment

( Coulomb’s Law )

Electric Force

Page 6: Equipment

Meet the Electron

Page 7: Equipment

Meet the Proton

QP = -Qe MP 2000•Me

Page 8: Equipment

Meet the Neutron

QN = 0 MN MP 2000 Me

0

Page 9: Equipment

Alpha ‘Particle’

0

0

Page 10: Equipment

Why does an alpha attract an electron?

Which is more (or are they equal): • the force on the alpha, or the force on the electron? • the acceleration of the alpha, or the acceleration of the electron?

Page 11: Equipment

The Electric Force• Have we ever actually seen evidence for

this force?• Can it be repulsive? How do you know?• Can this force be attractive? • Where is this force greatest (close or far)?• This force is strongest for highly charged

objects (why do we think this is true?).• How is this force like gravity, and how is it

different?

Page 12: Equipment

Electric Force Basics

• The force on object One equals the force on object Two. Recall the third law.

• The force is proportional to the charge of object One. F Q1

• The force is proportional to the charge of object Two. F Q2

• The force is proportional to the product of the charges: F Q1•Q2

Page 13: Equipment

Electric Force and Distance (R)

The farther apart the objects,the less the force.

F∝ 1

R2

Page 14: Equipment

Put all our ideas together

F ∝ Q1Q2R2

Page 15: Equipment

Change the proportionality to an equality by including a constant.

F = kQ1Q2R2

Hey, this looks familiar!

Page 16: Equipment

F = GM1M2

R2

Gravitation

Page 17: Equipment

k = 9.00 x 109 Nm2/C2

Let’s try an example:

One object has a charge of +0.5 Coulombs,and the other object has a charge of +2 C.

The objects are 3 meters apart.How much force repels these objects?

Show your buddy how to start this problem:

Page 18: Equipment

F = kQ1Q2R2

= (9 ×109)(0.5)(2)32

How much does this turn out to be, and what are the units?F = _____ Newtons. That’s a billion Newtons.

Page 19: Equipment

F = kQ1Q2R2

= (9 ×109)(0.5)(2)32

How much does this turn out to be, and what are the units?F = 109 Newtons. That’s a billion Newtons. This force is _ _ _ _.

Page 20: Equipment

F = kQ1Q2R2

= (9 ×109)(0.5)(2)32

How much does this turn out to be, and what are the units?F = 109 Newtons. That’s a billion Newtons. This force is huge. And a Coulomb is a _ _ _ _ amount of charge.

Page 21: Equipment

F = kQ1Q2R2

= (9 ×109)(0.5)(2)32

How much does this turn out to be, and what are the units?F = 109 Newtons. That’s a billion Newtons. This force is huge. And a Coulomb is a huge amount of charge.What would have been different if one of the charges was negative?

Page 22: Equipment

Electric Field (E)

• The electric field shows the direction that a charged object would be forced (if there was a positive charge at that spot).

• More intense fields are indicated by ‘lines’ that are drawn more densely…

Page 23: Equipment

Electric Field due to a positive point charge.

http://facstaff.gpc.edu/~pgore/PhysicalScience/electric-charge.html

Page 24: Equipment

Shape of the Electric Field

Page 25: Equipment

Electric Field due to a negative charge.

http://www.tutorvista.com/content/physics/physics-iv/electric-charges/electric-field-lines.php

Page 26: Equipment

Electric Field due to two positive charges.

http://www.tutorvista.com/content/physics/physics-iv/electric-charges/electric-field-lines.php

Page 27: Equipment

Electric Field due to a positive point charge and a negative point charge.

http://electron9.phys.utk.edu/phys136d/modules/m4/efield.htm

Page 28: Equipment

Shape of the Electric Field

http://web.ncf.ca/ch865/englishdescr/3DEFldDipole.html

Page 29: Equipment

Electric Field due to a oppositely charged parallel plates (edge view).

http://en.wikibooks.org/wiki/FHSST_Physics/Electrostatics/Electric_Fields

Page 30: Equipment

Shape of the Electric Field

http://web.ncf.ca/ch865/englishdescr/EFld2Plates.html

Page 31: Equipment

Basics of Electric Field Strength• To test the electric field at a point in space, put a

small charged object at that location. Likely there will be a force on the object (due to the other charges in the universe). If there is a force on the object, then there is an electric field at that point.

• If you doubled the charge of our “test charge”, the force on it would double. The strength of the field does not depend on the charge of the test object.

• If you didn’t bother to put a charge at the point, there would still be a field there (but no force).

Page 32: Equipment

There is no electric field inside a conductor.

http://electron9.phys.utk.edu/phys136d/modules/m5/conductor.htm

This happens because electrons in a conductor are free to move, so if there was an electric field

then charges would be forced to move to aposition until there was no more field.

Page 33: Equipment

The Strength of the Electric Field

E = F / q

Field = Force / Charge

The uptight definition of the Electric Field requires that q be positive:

E = limq0 F / q

Page 34: Equipment

One.How much force acts on ?

+4 C+2 C

3 meters

Page 35: Equipment

How much force acts on ?

• F = kQq ÷ D2 • F = (9x109)(2)(4) ÷ 32 • F = 8 x 109 N• In what direction is the force on ?

Page 36: Equipment

What is the value of theElectric field at ?

• E = F / q• E = (8 x 109 N) ÷ ?• E = (8 x 109 N) ÷ (4 C)• E = 2 x 109 units? • E = 2 x 109 N / C

Page 37: Equipment

What is the direction of theElectric field at ?

• Vital Definition: The direction of E at a point is the same as the direction that a positive charge would be forced if it was at that point.

• In this case, since is a positive charge that is forced to the right, the Electric field is to the Right.

Page 38: Equipment

Two.Find the force on and the Electric field at .

-3 C+2 C

3 meters

Page 39: Equipment

Find F and E.

• F = kQq/D2 • F = (9x109)(2)(-3) ÷ 32 • F = -6 x 109 N (towards the left)

• E = F/q = (-6x109) ÷ (-3) • E = 2x109N/C (towards right)• Compare to the first question (!) …

Page 40: Equipment

Why do the E’s have the same magnitude and direction?

+4 C+2 C

3 meters

One

Two

-3 C+2 C

3 meters

Page 41: Equipment

In the previous question, we found out that:

• The force depends on both charges, but• The Electric field depends on the charge that is

not at the spot that we are looking at.• E = F ÷ q • E = (kQq/D2) ÷ q • E = kQ ÷ D2 (the q at the spot cancels).

Page 42: Equipment

Three. What is the E at theempty spot (x) ?

x+5 C

6 meters

Page 43: Equipment

Two ways to find E.

• Slow: make up a value for q (at x) and calculate force. Then use E = F ÷ q.

• Faster, use E = kQ ÷ D2 • E = (9x109)(5) ÷ 62 • E = 1.25 x 109 N/C

Page 44: Equipment

Four. What is the E at theempty spot (x) ?

xQ

D

Page 45: Equipment

E = kQ ÷ D2


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