Transcript
Page 1: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

Physics 222 Exam Review

Page 2: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

Outline

ā€¢ Overview/Mind-mapā€¢ What each equation doesā€¢ Practice Problems

Page 3: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

Sorry about the boring theme.

ā€¢ I couldnā€™t find a suitable theme that I liked, that didnā€™t mess up my text.

ā€¢ However, looking at green is said to increase creativity and stimulate brain function. May use this later.

Page 4: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

Useful tip: Storing variables in calculator

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Charge

Electric Force

Electric Field

Potential EnergyElectric Potential

Divide by q

Multiply by q

Dipole

Interacts with dipole

Capacitors

Resistors

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Overview

ā€¢ Fluidsā€¢ Electric force -> Electric fieldā€¢ Potential energy -> Electric potentialā€¢ E->V and V->Eā€¢ Capacitors and energy stored inside themā€¢ Resistors

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š‘ƒ=š¹š“

ā€¢ This is the definition of Pressure: Force/Area

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š‘ƒ=š‘ƒ0+šœŒš‘”š‘¦ā€¢ Used to calculate the pressure at a depth of y

in some medium, usually water.ā€¢ Example: 5 m deep under the water, pressure=

Page 9: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

š‘‘š‘‰š‘‘š‘”

=š“š‘£=š‘š‘œš‘›š‘ š‘”š‘Žš‘›š‘”

ā€¢ This is the continuity equation for fluid flow.ā€¢ In English, it means that the amount of stuff

going through a pipe is constant, so shrinking the pipe means that the water will go faster.

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š‘ƒ+šœŒš‘”š‘¦+12šœŒš‘£2=š‘š‘œš‘›š‘ š‘”š‘Žš‘›š‘”

ā€¢ Also known as Bernoulliā€™s Equationā€¢ Classic problem: calculating velocity of water

shooting out of a hole in a container.ā€“ In the case that the radius of the hole is small, the

velocity at the bottom simplifies to where y is the distance from the water level to the hole.

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Questions?

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š‘­ š¶š‘œš‘¢š‘™š‘œš‘šš‘=š‘˜š‘’

š‘ž1š‘ž2š‘Ÿ2

ļæ½Ģ‚ļæ½

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š‘¬=š‘­š‘ž0

ā€¢ Just like electric force, but without the test charge q0. Itā€™s still a vector.

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š‘¬=š‘˜š‘’š‘žš‘Ÿ 2ļæ½Ģ‚ļæ½

ā€¢ Electric field of a point charge.

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Electric field lines go from + to -.

ā€¢ Also, line density indicates field strength

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š’‘=Ā暝‘„āˆØš’…ā€¢ Dipole moment, BY DEFINITIONā€¢ Notice: Dipole moment points from negative

to positiveā€¦.opposite of the direction E points

Page 17: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

š‰=š’‘Ć—š‘¬ā€¢ Torque on a dipole by the external electric

fieldā€“ Note that E is not the E produced by the dipoleā€“ E is external

ā€¢ Torque is maximum when dipole moment and E are perpendicular.

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š‘ˆ=āˆ’š’‘ ā‹…š‘¬ā€¢ Potential energy is minimum (also called stable

equilibrium) when two things are true:ā€“ Dipole moment is parallel to Eā€“ Dipole moment points in the same direction as E.

ā€¢ Potential energy is maximum (also called unstable equilibrium) when two things are true:ā€“ Dipole moment is parallel to E.ā€“ Dipole moment points in the opposite direction as E.

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Questions?

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ā€¢ Also known as Gaussā€™s Lawā€¢ Really there are two equations hereā€¦but

theyā€™re both equally validā€¦always.

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Steps in solving Gaussā€™s Law Problems

ā€“ Draw a picture of the object. Pick a good Gaussian surface.

ā€“ Write down the expression of Gaussā€™s Law that involves the dot product between E and A. (If E is perpendicular to A, the flux is 0 for that surface. Otherwise, use symmetry to get rid of the integral.)

ā€“ Write down the expression of Gaussā€™s Law that involves the total charge q.

ā€“ Set the two expressions equal to each other and eliminate variables.

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šø=š‘˜š‘’2šœ†š‘Ÿ

ļæ½Ģ‚ļæ½

ā€¢ Electric field a distance r away from a long wire with charge density .

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š‘¬=Ā±šœŽ2šœ–

ļæ½Ģ‚ļæ½

ā€¢ This one is especially important.ā€¢ This is the electric field anywhere away from a

large sheet of charge.ā€¢ Notice that the electric field doesnā€™t depend

on distance, and always points perpendicular to the surface.

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ā€¢ Classic problem: What is the electric field between two parallel plates of charge Q and area A?

ā€¢ Answer: Since you have two plates of opposite charge, the E fields add, and thusā€¦

ā€¢

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ā€¢ These relations let you go from either E to V or vice-versa. If you know one, you can calculate the other.

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š‘Š=āˆ’ Ī”š‘ˆ=āˆ’š‘ž0 Ī”š‘‰This equation can be used to:ā€¢ If youā€™re given you can find the work done.ā€¢ If a point charge of charge q0 goes through a

potential difference of it tells you the work done on the charge.

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š‘ˆ=š‘ž0š‘‰ā€¢ This is the defining relation between potential

energy (U) and electric potential (V).ā€¢ Note: since q0 can be positive or negative, U

and V do not necessarily have the same sign.ā€¢ One more time: Electric potential (V) is not the

same thing as electric potential energy (U)ā€¢ But letā€™s rewrite it.

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š‘‰=š‘ˆ /š‘ž0Similar to: .

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š‘‰=š‘˜š‘’š‘žš‘Ÿ

ā€¢ Electric potential of a point charge q, a distance r away, assuming V=0 at infinity.

ā€¢ Potential goes up as you get closer to the point charge.

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Ī”š‘‰=Ā±šøš‘‘ā€¢ Rather important: This is the potential

difference between two parallel conducting plates, otherwise known as a capacitor.

ā€¢ What is E for a capacitor again?

Page 31: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

š¶=š‘„š‘‰

ā€¢ Definition of capacitanceā€¢ C=Charge Q/ Voltage drop

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š¶=šœ–0š“š‘‘

ā€¢ Special case of capacitance when youā€™re looking at a parallel plate capacitor.

ā€¢ Notice that the capacitance doesnā€™t depend on the charge on the plates.

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š¶š‘’š‘ž=š¶1+š¶2+ā€¦ā€¢ Adding capacitors in PARALLEL.

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1š¶š‘’š‘ž

=1š¶1

+1š¶2

+ā€¦

ā€¢ Adding capacitors in SERIES.

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š¶=4 šœ‹šœ–0š‘Žš‘š‘āˆ’š‘Ž

ā€¢ Special case of capacitance when youā€™re looking at a two concentric spherical conducting shells.

ā€¢ The radius of the smaller shell is a, the radius of the larger shell is b.

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š¶=4 šœ‹šœ–0š‘…ā€¢ The capacitance of a single spherical shell of

radius R

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š‘ˆ=12š¶š‘‰ 2= š‘„2

2š¶=12š‘„š‘‰

ā€¢ You use these equations to calculate the stored energy in a capacitor

ā€¢ Okay, but thereā€™s 3 different equations, so which one is appropriate for my problem?ā€“ If they just ask you to calculate U, use the one that

has variables you know.ā€“ If they ask you what happens to U if you double the

charge, halve d, etcā€¦ā€¢ If the capacitors are stand-alone, use .ā€¢ If the capacitors are connected to a voltage source, use

Page 38: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

šœ–=šœ…šœ–0ā€¢ This relates the permittivity of free space to

the permittivity in a medium of dielectric constant .

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š¶=šœ…C0ā€¢ Relates capacitance without a dielectric (C0) to

capacitance with a dielectric.

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š‘¢=12šœ–šø2

ā€¢ The energy density when you have an electric field E in a medium of permittivity

ā€¢ For example, letā€™s say you have a cube (L=3) filled with water (. The cube has the same E field everywhere (E=5). ā€“ Then u=ā€“ Total stored energy=

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š¼=š‘‘š‘„š‘‘š‘”

ā€¢ Definition of current.

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š‘‰=š¼š‘…ā€¢ Ohmā€™s Law: A relationship between voltage,

current, and resistance.ā€¢ Pretty fundamental.

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š½=š¼š“

=š‘žš‘›š‘£š‘‘

ā€¢ =Current densityā€¢ n = density of charge carriersā€¢ Vd=drift velocity (average velocity of charge

carriers)ā€¢ q=charge on a charge carrier (usually e=

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šø= š½ šœŒā€¢ Microscopic Ohmā€™s Law:ā€¢ E-field (E) = Current density (J) x resistivity (

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š‘…=šœŒšæš“

ā€¢ Resistance of a conductor of resistivity , length L, and cross-sectional area A

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šœŒ=šœŒ0 (1+š›¼ (š‘‡ āˆ’š‘‡0 ) )ā€¢ Resistivity changes as a function of

temperature.

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š‘…=š‘…0 (1+š›¼ (š‘‡ āˆ’š‘‡ 0 ))ā€¢ Resistance changes as a function of

temperature

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š‘…š‘’š‘ž=š‘…1+š‘…2+ā€¦ā€¢ Adding resistances in series.

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1š‘…š‘’š‘ž

=1š‘…1

+1š‘…2

+ā€¦

ā€¢ Adding resistances in parallel.

Page 50: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

Practice Problems

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Page 58: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

In the figure to the right, there are two charges connected by a massless insulating rodā€¦and remember to use VECTORS when appropriateā€¦Draw the electric dipole.

Torque caused by the electric field=

Dipole moment=

Potential energy as it is right now=

Which way will the dipole begin to rotate? (Clockwise/Counter-clockwise)

How much work is done in rotating the dipole from its current position to the stable equilibrium position?

What does the work in question f?

Page 59: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

A block of MagicFoam (length 10 cm, width 10 cm, height 3 cm) sits on top of a calm body of water. MagiFoam density=0.5 g/cm3. How much of the block is submerged?

A 10 kg block floats in the water. What is the buoyant force on it?

A house with a roof of area 5 m2 has winds of 50 m/s above it. What is the force on the roof caused by the pressure difference?

Page 60: Physics 222 Exam Review. Outline Overview/Mind-map What each equation does Practice Problems

How much energy does it take to bring two electrons within .1 n of each other?

Some water is flowing at a rate of 20 mph in a pipe. Further on in the pipe, the pipe halves its diameter. What is the new speed of the water?

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If current is going from your hand to your foot, which direction are

the electrons going?

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Final Questions?

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Thank you, and good luck!


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