D2 Electric and Magnetic Fields

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Electro + Magnetic

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24 Terms

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D2.1 Electric charge

Charge is property of matter, responsible for electric force.

Unit: Coulomb (C): charge carried by electric current of 1A in 1s

Symbol: q

Quantisation: matter is made of atoms, which are made of:
1. Electrons: -1 charge
2. Protons: +1 charge
3. Neutrons: neutral (0 charge)

Most everyday object have charge = 0; protons/electron have magnitude of charge = elementary charge = e = 1.60 ×10-19C

Object becomes charged if there is an excess of protons or neutrons; always exactly +1 or -1 e so quantised.

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D2.2 Electric Forces

When 2 charges are close tg. They exert a force on each other:
Attractive: closer tg. : unlike charges: opposites attract
Repulsive: further ap. : like charges

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D2.3 Conservation of charge

Charge is conserved: total charge in isolated system in constant

charge can be transferred, but not created nor destroyed.

REMEMBER THIS IN NUCLEAR DECAY!!

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D2.4 Millikan’s Oil Drop

Determined value of elementary charge.
Oil used instead of water so no evap, no Δm.

Oil drops sprayed out into chamber and charged by friction by falling; some drops lose e- and become + charged, and vice versa. The drops passes 2 metal plates and is viewed under microscope.

Usually, the drop falls under gravity, reaching terminal velocity (air resist.) However, with the inclusion of electric field; potential diff is applied between metal plates → electric field. Charged drops rise when field is strong enough. Felectric> Fg
F = Eq (F=electrostatic F on charge NC-1) (E=electric field strength;N)(q=charge; C).

Found e = 1.6 × 10-19 C

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C2.5 Charge transfer by friction

Friction: when 2 insulators (no free e-) are rubbed tg. One +change, one - : rod+cloth; e- rod→ cloth. Discharged when in contact with another insulator

<p>Friction: when 2 insulators (no free e<sup>-</sup>) are rubbed tg. One +change, one - : rod+cloth; e<sup>-</sup>  rod→ cloth. Discharged when in contact with another insulator<br></p>
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C2.6 Electrostatic induction

Seperation of charge; put uncharged object close to charged one;

Eg. Balloon next to negatively charged rod: electron move to opposite end. When then grounding, electrons leave and balloon is left with + charge on it, even when removing the rod.

<p>Seperation of charge; put uncharged object close to charged one;</p><p>Eg. Balloon next to negatively charged rod: electron move to opposite end. When then grounding, electrons leave and balloon is left with + charge on it, even when removing the rod. </p>
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C2.7 Charge by contact

From charged insulator to earther conducto: large potential diff.

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C2.8 Insulator conductor

Conductor: freeflowing e-: metals + graphite

Insulator: plastic, glass, dry wood.

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C2.9 Dangers of static electricity

When potential diff between 2 object become VERY large; E field strong enough to intract w air causing current in air →spark

Electrocution: lightning

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D2.10 Coulomb’s Law

All q’s generate an electric field → F on nearby q’s.
Electric F between 2 point charges ∝ q1q2 (charge) and 1/r2 (sep)

F = kq1q2/r2 (k = 8.99 ×109) (q in C!!!) -

k = 1/4πε0

ε0 = Permittivity of free space = 8.85 × 10–12 (measure of resistance offered by material in creating an electric field in it)

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D2.11 Repulsive/Attractive F

Can be either attractive or repulsive: depends on q’s

both +, or both -: +Force → repulsive

one + one -: - Force → repulsive

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D2.12 Electric Field Strength

Force per unit charge experienced by small + test charge placed at that point.
E = F/q = kq/r2
+q: experience force Eq in direction of field
-q: experiences force Eq in opposite direction

Away from + charge, Towards - charge

Charged sphere acts as point charge, w same charge as sphere at centre, within sphere, E = 0 untiil surface, then start decreasing as a 1/x graph.

Can add them up like vectors (keep direction in mind).
Resultant field depends on type and magnitude of charges

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D2.13 Electric Field between Parallel Plates

E = V/d (d=sep between plates)(V = potential diff between plat)

Greater V → stronger F, Greater d → weaker F
NOT FOR POINT CHARGES!!!! Radial vs parralel fields.
Field goes from + plate (+ terminal) to the - plate (- terminal)

<p>E = <sup>V</sup>/<sub>d</sub> (d=sep between plates)(V = potential diff between plat)</p><p>Greater V → stronger F, Greater d → weaker F<br>NOT FOR POINT CHARGES!!!! Radial vs parralel fields. <br>Field goes from + plate (+ terminal) to the - plate (- terminal)</p>
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D2.14 Electric field lines

Direction + magnitude of field experienced by + test charge:

ALWAYS directed from + charge to - charge (experienced by the + charge)

  • + charge: away

  • - charge: towards

Strength of field is strongest: lines closest tg, weakest: furthest…

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D2.15 E - field between 2 point charges

2 opposite: from + to -
2 same: repelling, either to (-), or from (+) - neutral in middle

<p>2 opposite: from + to -<br>2 same: repelling, either to  (-), or from (+) - neutral in middle</p>
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D2.16 Electric Potential

Wok done per unit charge in taking + test charge from ∞ → point

J C-1 = V. At infinity → 0

Around a + charge: + value, requires work to get here, V decreases (to 0) with moving further away

Around a - charge: - value, requires work to move away, V increase (to 0) with moving further away.

Ve = kQ/r (Q of charge producing potential.

Inside charged sphere, V = constant (not 0)
V = kQ1/r1 + kQ2/r2

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D2.17 Electric Potential Energy

Work done in bringing all charge in system to position from ∞.
like charges: repulsive F; +Ep : energy released in seperating
opposite charges: attractive F: -Ep : energy supplied to seperate

Ep = k(q1q2)/r = change in Ep = W= FΔr (area under Fr graph)

ΔEp = kq1q2 (1/r1 - 1/r2)

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D2.18 Graphs…

E - r graph: area = V
F - r graph: area = E

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D2.19 Equipotential surfaces (electric)

Equipotential: equal electric potential; perp to electric field lines

Along surface; no Work done.

Dipole: ++/ --: rondjes, +-: lines outwardish. Closer to charge = larger field.

Uniform field: parallel lines

<p>Equipotential: equal electric potential; perp to electric field lines</p><p>Along surface; no Work done. </p><p>Dipole:  ++/ --: rondjes, +-: lines outwardish. Closer to charge = larger field.</p><p>Uniform field: parallel lines</p>
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D2.20 Magnetic Fields

Region of space in which magnetic pole experiences force

  • by moving electric charge

  • permanent magnets

magnetic field = B-field. Stat-charge doesnt produce field. Around current carrying wire. Invisible, but see effect pulling magnetic materials.

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D2.21 Magnetic Flux Density

Magnetic Flux Density: B: nr of magnetic field lines passing through region of space per unit area: Teslas (T) (force N on 1m wire carrying 1A at right angle to field)
higher B: stronger field: field lines closest

Direction + magnitude to represent them: N → S pole. Close tg at poles.

Around bar magnet, into/to South, out of/from North. nevr cross

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D2.22 Magnetic field between 2 bar

2 like poles: repel, 2 opp: attract

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D2.23 Right Hand Rule

Magnetic field around current carrying wire.
Thumb = current, Fingers = field

N = outward = puntje = anticlock

S = inward = cross = clock

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D2.24 Magnetic vs Electro

M: moving q’s, closed loops,

E: stationa q’s, start + end -,