chapter 18 electric forces and electric fields. 18.1 the origin of electricity the electrical nature...

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Chapter 18

Electric Forces and Electric Fields

18.1 The Origin of Electricity

The electrical nature of matter is inherentin atomic structure.

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coulombs

18.1 The Origin of Electricity

In nature, atoms are normallyfound with equal numbers of protonsand electrons, so they are electricallyneutral.

By adding or removing electronsfrom matter it will acquire a netelectric charge with magnitude equalto e times the number of electronsadded or removed, N.

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18.2 Charged Objects and the Electric Force

LAW OF CONSERVATION OF ELECTRIC CHARGE

During any process, the net electric charge of an isolated system remainsconstant (is conserved).

18.2 Charged Objects and the Electric Force

Like charges repel and unlike charges attract each other.

18.3 Conductors and Insulators

Not only can electric charge exist on an object, but it can also movethrough and object.

Substances that readily conduct electric charge are called electricalconductors.

Materials that conduct electric charge poorly are called electricalinsulators.

18.5 Coulomb’s Law

COULOMB’S LAW

The magnitude of the electrostatic force exerted by one point chargeon another point charge is directly proportional to the magnitude of the charges and inversely proportional to the square of the distance betweenthem.

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18.5 Coulomb’s Law

Example 4 Three Charges on a Line

Determine the magnitude and direction of the net force on q1.

18.5 Coulomb’s Law

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18.6 The Electric Field

DEFINITION OF ELECRIC FIELD

The electric field that exists at a point is the electrostatic force experiencedby a small test charge placed at that point divided by the charge itself:

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SI Units of Electric Field: newton per coulomb (N/C)

18.6 The Electric Field

Electric fields from different sourcesadd as vectors.

18.6 The Electric Field

Example 10 The Electric Field of a Point Charge

The isolated point charge of q=+15μC isin a vacuum. The test charge is 0.20m to the right and has a charge qo=+0.80μC.

Determine the electric field at point P.

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18.6 The Electric Field

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18.6 The Electric Field

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The electric field does not depend on the test charge.

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The electric field produced by apoint charge q:

18.6 The Electric Field

THE PARALLEL PLATE CAPACITOR

Electric field produced by a parallel platecapacitor

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18.7 Electric Field Lines

Electric field lines or lines of force provide a map of the electric fieldin the space surrounding electric charges.

18.7 Electric Field Lines

Electric field lines are always directed away from positive charges andtoward negative charges.

18.7 Electric Field Lines

Electric field lines always begin on a positive chargeand end on a negative charge and do not stop in midspace.

18.7 Electric Field Lines

The number of lines leaving a positive charge or entering a negative charge is proportional to the magnitude of the charge.

18.7 Electric Field Lines

18.9 Gauss’ Law

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18.9 Gauss’ Law

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18.9 Gauss’ Law

GAUSS’ LAW

The electric flux through a Gaussiansurface is equal to the net charge enclosed in that surface divided bythe permittivity of free space:

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SI Units of Electric Flux: N·m2/C

PROBLEMS TO BE SOLVED

• 18.20(21) [(a)0.166N,along +y-axis,(b)110.67m/s2,along +y-axis]; 18.35(36)[(a)8.02×105N/C,(b)1.28×10-13N]; 18.53(53)[32.55×10-9C].

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