chapter 17: electric potential 1. as in earlier chapters on mechanics we learned that energy is...

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Chapter 17: Electric Potential 1

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Page 1: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

Chapter 17: Electric Potential

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Page 2: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is transferred from one object to another or transformed into another type of energy

Energy and its interactions can help us understand nature

Work performed on a charged particle in an electric field can result in the particle gaining electric potential energy (PE), kinetic energy (KE) or both

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Page 3: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

The electric field does work when it moves the charged particle from location a to b

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Page 4: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

Electric potential is defined as the electric potential energy per unit charge and is measured with a voltmeter

Va= Electric Potential: Units=volt (V). Named after Alessandro Volta, inventor of the electric battery

PEa= Electric Potential Energy: Unit= joule (J)

q = Charge on particle: Unit=Coulomb (C)4

Page 5: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

Also called voltage Electric potential difference is the

difference in electric potential (V) between the final and initial position

Δ Also the ratio of work needed to move a

charge between two points divided by the magnitude of the charge

ΔV=W q

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Page 6: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

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Page 7: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.2 Relation between Electric Potential and Electric Field

A uniform electric field can made by placing two large flat conducting plates of opposite charge parallel to each other The electric field can be calculated by dividing the potential

difference between the plates by the distance between the plates (in meters)

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Page 8: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.3 Equipotential Lines Electric potential can be

represented by drawing equipotential lines (green)

An equipotential is a line over which the potential is constant

Equipotential lines are perpendicular to the Electric field (red)

Conductors are equipotential surfaces

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Page 9: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

The electric field is strongest where the equipotential lines are closest together.

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Page 10: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.4 The Electron Volt, a Unit of Energy

The joule is a large unit to deal with energies of electrons, atoms or molecules

The electron volt (eV) is used An eV is the energy gained by an electron

moving through a potential difference of one volt.

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Page 11: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.7 Capacitance A capacitor consists of two conductors

that are close but not touching. A capacitor has the ability to store electric charge

In general capacitance increases as the plates become larger and decreases as the separation between plates increases

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Page 12: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

Capacitors are used widely in electronic

circuitspower failure

back upsBlocking

surges of charge and energy

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Page 13: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

(a) Parallel-plate capacitor connected to battery. When connected to a battery the plates become charged; one + and one –

(b) In a circuit diagram the capacitor is represented as seen here

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Page 14: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

• C is the capacitance and depends on the size, shape, position and separating material of the capacitor

•Unit of capacitance: farad (F) 1 F = 1 C/V (coulomb/volt)

When a capacitor is connected to a battery, the amount of charge (Q) on its plates is proportional to the potential difference (voltage) between them

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Page 15: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.8 Dielectrics Most capacitors have an insulating sheet of between the plates

This insulator is a dielectric

Do not break down and allow charge to flow as easily as air, allowing higher voltages

Allow plates to be closer together

Increase the capacitance by a factor of K; a dielectric constant

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Page 16: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

If the electric field in a dielectric becomes too large, it can tear the electrons off the atoms, thereby enabling the material to conduct. This iscalled dielectric breakdown; the field at which this happens is called the dielectric strength

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Page 17: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

17.9 Storage of Electric Energy

A charged capacitor stores electric energy by separating + and – charges

The energy stored is equal to the work done to charge it

Stored energy in a capacitor can cause burns or shocks, even when the external power is off!

There are many uses for capacitors; a camera flash, a cardiac defibrillator, etc.

An essential part of most electrical devices used today 17

Page 18: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

A defibrillator is a capacitor charged to a high voltage. Once charged it sends a brief charge through the heart. This can stop the heart and (hopefully!) allow it to resume normal beating

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Page 19: Chapter 17: Electric Potential 1.  As in earlier chapters on mechanics we learned that energy is conserved; it is neither created nor destroyed but is

Zitewitz. Physics: Principles and Problems. 2004

Giancoli, Douglas. Physics: Principles with Applications 6th Edition. 2009.

Walker, James. AP Physics, 4th Edition. 2010

http://commons.wikimedia.org/wiki/File:Capacitor_schematic_with_dielectric.svg

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