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Stream lines. front plate slightly charged induces opposite charge on back plate. Brushes pull off charges charges collected in leyden jar (capacitor)

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Presentation on theme: "Stream lines. front plate slightly charged induces opposite charge on back plate. Brushes pull off charges charges collected in leyden jar (capacitor)"— Presentation transcript:

1 Stream lines

2 front plate slightly charged induces opposite charge on back plate. Brushes pull off charges charges collected in leyden jar (capacitor)

3 Electric Field

4 Definition Electric field is the strength & direction of the forces in space surrounding a positive test charge

5 Electric field as coulomb’s law F = q 1 * (k q 2 /d 2 ) rewrite the force equation F = q 1 * E q 1 is the positive test charge E is the field created by charge(s) q 2

6 Top tips on electric field E=0 inside a metal (faraday) cage Field lines go from + to – charges Closer field lines are stronger

7 Electric Field between 2 unlike charges + - A B C Note that the distance between electric field lines at C is shorter than that at B. Distance between electric field lines at B is shorter than at A.

8 Electric Field between 2 charged plates positive negative

9 Electric Field between 2 charged plates ++++ ++++ ---- ----

10 coulombs, joules, volts Coulomb= unit of charge Joule = unit of energy Volt= unit of energy per charge

11 coulomb How many charges are in 1C? coulomb? 1C is about 6 billion billion charges) (1/1.6 x 10 -19 = 6.25 x 10 18 ) The man, the law Charles Coulomb~1750

12 Joulesof energy Charges have a type of energy called electron potential energy (PE e or U) High energy: + is close to +: ++ or + is far from –: + -

13 It takes work to move charges against (opposite) an electric field High energy work needed to move + charge (W = F*d) E F + low energy

14 POSITIVE charge moving in an E field. (a) When a positive charge moves in the direction of an electric field, the field does positive work and the potential energy decreases. Work = q o E d

15 Volts is an energy density Voltage is also called potential 1 volt = 1 joule / 1 coulomb Example: 12 V battery: every coulomb of charge has 12 joules of energy

16 Examples Static balloon 9 V battery (1hr,1A) 1 joule of energy 9x10 4 joule energy 0.001 C of charge 1x10 4 C of charge 1/.0001 = 1000 volts 9/1 = 9 Volts

17 Another c,j,v example Van de graaf static generator has.. 1,000,00 volts (high) 1 joule of energy (low).00001 coulombs of charge 1,000,000 v = 1 j/.00001c

18 Uniform electric field2 situationsPoint Charges Force:F=q*EForce= k q 1 *q 2 / d 2Electric potential energy PE= F*d = q*E*dPE = F*d = k q 1 *q 2 / d Voltage (electric potential) V= PE/q 1 = q*E*d /q = E*d V= PE/q 1 = k q 2 / d 2 Voltage difference:  Ve =  PE/q 1 = E*  d  Ve =  PE/q 1 = k q 2 / d 2 - kq 2 / d 1

19 It takes work to move + charge against static forces like it takes work to lift against gravity PE final +++++ + Pe iniitial work = gain in PE = F*d

20 Electrostaticsgravitational Force: F= kq 1 q 2 / d 2 F= Gm 1 m 2 /d 2 Field E= F/q 1 = kq 2 /d 2 g = F/m 1 = Gm 1 /d 2 potential energy PE= F*d = kq 1 q 2 / dPE = F*d= Gm 1 m 2 /d (using field) =qE*d = mg*h Potential V= PE/q 1 = kq 2 / dU= PE/m 1 = G m 2 / d (Using field) = E*d = g*h


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