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Electricity Charge and Field Presentation 2003 R. McDermott
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Page 1: Electricity Charge and Field Presentation 2003 R. McDermott.

Electricity

Charge and Field

Presentation 2003 R. McDermott

Page 2: Electricity Charge and Field Presentation 2003 R. McDermott.

Static Electricity

• Non-moving charges.• Characteristic of insulators.• Positive and negative charges.• Protons in a solid can’t move.• Changes in charge are due to electron

transfer.• Friction produces static electricity.

Page 3: Electricity Charge and Field Presentation 2003 R. McDermott.

Two Kinds of Charge

• Unlike charges attract

• Like charges repel

• Both charges attract neutral objects

• Removing electrons results in positive charge (silk on glass).

• Adding electrons results in negative charge (fur on plastic).

Page 4: Electricity Charge and Field Presentation 2003 R. McDermott.

Conservation of Charge

• Total charge is constant.• Electrons transfer from more negative to less negative

object.• Most everyday objects are neutral (most atoms are

neutral).• Identical objects in contact develop the same charge.

Page 5: Electricity Charge and Field Presentation 2003 R. McDermott.

Atoms Contain Charge

• Protons inside nucleus are positive.

• Electrons outside nucleus are negative.

• Proton and electron have same charge magnitude.

• Electrons can move within solid material

Page 6: Electricity Charge and Field Presentation 2003 R. McDermott.

The Smallest Charge

• The charge on an electron (-1), or proton (+1) is one “elementary” charge.

• Which equals 1.602 x 10-19 Coulombs• Charge is quantized• Discrete amounts only• 1e, 2e, 3e, 4e etc• Quarks of sub-atomic physics have -1/3

and +2/3 charge

Page 7: Electricity Charge and Field Presentation 2003 R. McDermott.

Producing Localized Charges

• Rubbing

• Inducing a nonsymmetrical charge distribution.

• Conduction

• Grounding (Induction)– Connect with wire

leading to ground

Page 8: Electricity Charge and Field Presentation 2003 R. McDermott.

Inducing a nonsymmetrical charge distribution.

In the picture to the right, a negatively charged rod brought close causes electrons in the object to move away (downward).

Even though the object is still neutral, its top is now slightly positive, and its leaves slightly negative as a result.

Page 9: Electricity Charge and Field Presentation 2003 R. McDermott.

Inducing a nonsymmetrical charge distribution.

In the picture to the right, a positively charged rod brought close causes electrons in the object to move toward it (upward).

Even though the object is still neutral, its top is now slightly negative, and its leaves slightly positive as a result.

Page 10: Electricity Charge and Field Presentation 2003 R. McDermott.

Charging by Conduction

• An object is charged by conduction if you touch a charged object to it, allowing electrons to be transferred.

• Using a negative object results in a negative charge. Using a positive object results in a positive charge, as shown to the right:

Page 11: Electricity Charge and Field Presentation 2003 R. McDermott.

Charging by Induction

• An object is charged by induction if you touch a neutral object (ground) to it, while holding a charged object nearby.

• Using a negative object results in a positive charge. Using a positive object results in a negative charge, as shown to the right:

Page 12: Electricity Charge and Field Presentation 2003 R. McDermott.

Electroscope

• Detects charge with leaves that repel or needle that rotates.

Page 13: Electricity Charge and Field Presentation 2003 R. McDermott.

Charging by Induction

Page 14: Electricity Charge and Field Presentation 2003 R. McDermott.

Charging by Induction

Page 15: Electricity Charge and Field Presentation 2003 R. McDermott.

Insulators and Conductors

• Conductors carry charge easily– Metals have many free electrons– Ionic liquids– Plasmas

• Insulators conduct poorly– Dry gases– Wood, paper, cloth, glass, etc

• Semiconductors (silicon, germanium) are insulators that can be altered to conduct.

Page 16: Electricity Charge and Field Presentation 2003 R. McDermott.

Coulomb’s Law

• Electric force is proportional to product of charges divided by square of distance between them

• Q in coulombs• k is Coulomb constant• k = 8.988x109 Nm2/C2

• constant is the permittivity of free space• Applies to point charges

Page 17: Electricity Charge and Field Presentation 2003 R. McDermott.

Example 1 – Calculate Coulomb Force

• Find the force between two objects with charge 1 Coulomb at a separation of one meter.

• If their mass is 1 kg each, what is the gravitational force between them?

• How do the two forces compare?

Ans. 9x109 N

Ans. 6.7x10-11 N

Page 18: Electricity Charge and Field Presentation 2003 R. McDermott.

Example 2

• Find force between two, 1 -coulomb (10-6 coulomb) charges at separation of 20 cm

F = kQ1Q2/r2

F = (9x109 N-m2/C2)(1x10-6 C)(1x10-6 C)/(0.20 m)2

F = 0.225 N

Page 19: Electricity Charge and Field Presentation 2003 R. McDermott.

Electrostatic Force and Vectors

• Fnet = F1 + F2 + F3 + …

• Principle of superposition of forces

• Use component method of vector addition

• Fx = F1x + F2x Fy = F1y + F2y

Page 20: Electricity Charge and Field Presentation 2003 R. McDermott.

Recall:

• F1x = F1cos

• F1y = F1sin

• F = (F1 + F2)1/2

• TanFy/Fx

Page 21: Electricity Charge and Field Presentation 2003 R. McDermott.

Electric Field

• Force acting at a distance vs. field concept.

• Field, E, at a point is the force on a positive charge at that point divided by magnitude of that charge.

• Direction is the same as the direction of the force on a positive charge.

• The spacing of field lines indicates the strength of E.

Page 22: Electricity Charge and Field Presentation 2003 R. McDermott.

Electric Field Strength

• Units: newtons per coulomb

• Defined as E = F/q

• E = kQ/r2 is the field strength due to a point charge Q as measured at some point ‘r’ from Q.

Page 23: Electricity Charge and Field Presentation 2003 R. McDermott.

Problem Solving

• Draw careful diagrams• Apply Coulomb’s Law to get magnitude of

forces or fields• Determine direction of forces by considering

like and unlike charges• Show and label each vector force or field• Add vectorially to get resultant• Use symmetry when possible

Page 24: Electricity Charge and Field Presentation 2003 R. McDermott.

Three Charges in a Line

• Each charge will experience two electric fields and therefore two forces; one from each of the other two charges.

• The net field (and force) will be the vector sum of those two fields (and forces).

Page 27: Electricity Charge and Field Presentation 2003 R. McDermott.

Fields and Conductors

• Field inside conductor is zero.• If not, force F=qE would make charges move.• Charge spreads out optimally on surface.• Charge +Q inside spherical uncharged shell

induces -Q on inside surface of shell.• +Q then exists on outside surface of shell.• Electric field just outside a conductor is

always perpendicular to the surface.

Page 28: Electricity Charge and Field Presentation 2003 R. McDermott.

Acknowledgements

• Zoomschool.com

• Glenbrook South Physics

• Fizzics Fizzle at Thinkquest.com

• Dr. Philip M. Dauber