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100 Volts 0 Volts v o,x
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x V(x) 50 150 100 200 50 Volts 200 Volts
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-200 Volts 200 Volts z y coordinates x
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10 V 0 V (note the perpendicular intersections)
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10 V 0 V x y (line of symmetry is x-axis where y=0)
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3 V 0 V x y x V(x,0) yields 10 5 0 7 V 10 V (where the equipotential line intersects the line of symmetry)
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x (cm) V(x,0) yields 10 5 0 E x (x,0) 150 75 0 x (cm)
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x U(x) potential energy stable equilibrium (F NET = 0) unstable equilibrium (F NET = 0) negative slope (F NET to right) positive slope (F NET to left) AB CD
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x U(x) potential energy A: stable equilibrium C: unstable Equilibrium D: F NET to right B: F NET to left AB CD
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x U(x) potential energy AB CD
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x V(x) electric potential AB begin
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x y + Radial electric vector field of a charged conducting circle
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x y + x y _
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_ x y
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x y _
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y U(x,y) potential energy F NET to right and forward) x dotted lines show constant energy
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y U(x,y) potential energy F NET to right and forward) x (dotted lines show constant energy: “equipotentials”) (equipotentials closer where steepest)
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y V(x,y) electric potential (potential energy per unit charge) E(x,y) x dotted lines show constant electric potential + + solid lines show electric field arrow shows electric field direction on positive test charge
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y V(x,y) x (dotted lines show constant electric potential) + + (solid lines show electric field) (arrow shows force on test charge) + +
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y V(x,y) Electrical potential energy per unit charge x (equipotentials closer where steepest) + (dotted lines show constant electric potential while solid lines show electric field)
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y V(x,y) x (dotted lines show constant electric potential) + (solid lines show electric field)
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y V(x,y) x dotted lines show constant electric potential + solid lines show electric field
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y x +
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x y
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x y V=4 volts A B q
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V=7 volts V=5 volts E=?
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V=7 volts V=5 volts E=? d = 2 cm
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100 V/m x y = 35 o must be estimated or measured with a protractor to calculate the legs (x and Y components of E). 57 V/m 82 V/m
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10 o 15 o 30 o 45 o 60 o 75 o
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y V(x,y) E(x,y) x dotted lines show constant electric potential _ + solid lines show electric field arrow shows electric field direction on positive test charge
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y V(x,y) x _ +
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+ ++ + + ++ + + ++ + + ++ + + ++ + + ++ + + + +
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V I L A CROSS SECTION
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BATTERY + + I TOTAL IAIA IBIB ICIC IEIE IDID BATTERY + +
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+ PUMP (handle) (spinning paddle wheel) e e ee e e e e e e e e e e e
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R V source RR R a bc d e fg h
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R R R resistors in series R V source R resistors in parallel R V source
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6 3 V 6
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BATTERY + the ground BATTERY + the ground current can never flowcurrent may flow (depending on the properties of the ground)
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BATTERY + the ground
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9-VOLT BATTERY + _ 9-VOLT BATTERY + _
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+ -
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NS NS Unmagnetized iron filings before being placed in magnetic field. S N SN S N
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NS compass ? Needle direction? Draw needle in compass circle.
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STOP PRELAB
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- - - -- - -- - + + + + + +
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Uncharged conducting coin grounded to Earth.
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+ - - - - -- - - The presence of positive charge creates an electric field at the coin surface that attracts electrons from the Earth to negatively charge the coin.
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+ - -- - Removing the grounding wire leaves the coin positively charged. The Earth is a giant reservoir of charge, we do not worry about the fact that it has some miniscule amount of excess positive charge.
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+ - -- - The presence of positive charge creates an electric field at the coin surface that causes macroscopic charge separation. (The coins positive charges are forced to be far away from the positively charged object.) + + + +
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+ - -- - + + + +
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L E O N E + - -- - If some fool’s hand comes into contact with the coin, the coin’s positive charges can move even further from the charged object by moving into the hand (and body). + + + +
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L E O N E + - -- - + + + +
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+ - -- - Removal of the hand leaves a negatively charged coin. The hand is a large reservoir of charge and we will not worry about the miniscule amount of excess positive charge in the hand (and body) unless a very strong electric field had been present.
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+ - -- - In presence of positively charged object.Positively charged object removed. ?
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1.5 V A.B. C. 1.5 V D. 1.5 V V V + - + - V + - V + - V + - E.
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6.0 V a b 4.5 V A.B. 6.0 V B.A. 6.0 V
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a b c d 4.5 V A.B. 7.5 V 4.5 V B. A. 7.5 V 4.5 V
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6.0 V a b c d 4.5 V A.B. 7.5 V 4.5 V B. A. 7.5 V 4.5 V
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pith ball (conductor) + Initial attraction + repulsion after touching
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metallic enclosure solid metallic bar with round end very thin strip of pure gold
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+ + + + + + + + +
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+ _ _ + + _ + _ + _ + _ + _ + _ + _ _ + _ + _ + _ + _ + _ _
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BATTERY + +
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R V source R R R R A.B.C.
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BATTERY + + + + V 1.5 0 3.0 4.5 6.0
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- - - -- - -- - + + + + + + - - - -- - -- - balloon sticks to wall
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+ - -- - + + + +
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R V source R R
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+ _ _ point of intersection
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+ _ _ point of intersection can’t happen
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+ - - + - + A BC
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V R1R1 R2R2 V R equivalent
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V R1R1 R2R2 V
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6 V 1
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9 V 1 2 4 9 V RARA 4 9 V RBRB
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10 V R 1 = 1 R 2 =4 I 2 =? V 2 =? I 1 =? V 1 =?I Battery =?
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12 V R 1 = 5 R 2 =1 I 2 =? V 2 =? I 1 =? V 1 =?I Battery =? R Total = ?
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10 V R1R1 R2R2 RARA
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9 V R 1 = 1 R 2 = 2 R 3 =4 I 3 =? V 3 =? I 1 =? V 1 =?I 2 =? V 2 =?I Battery =?
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10 V R 1 = 8 R 2 = 8 R 4 =2 I 4 =? V 4 =? I 1 =? V 1 =? I 2 =? V 2 =?I Battery =? R 3 =2 I 3 =? V 3 =? R total = 5 ohms I battery = 2 amps V 1 = V 2 = 8 volts I 1 = I 2 = 1 amp V 3 = V 4 = 2 volts I 3 = I 4 = 1 amp
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R V applied
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I
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V 100 abc 200 V a c b 100 d ef
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V 200 a c b 100 d ef
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R
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200 100 red 1 black 2 red 2 + - black 1
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tV(t) 5 0 -5 tt
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I V applied
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12 V R 1 = 8 I 1 =? V 1 =? I Battery =? R 2 =1 R equivalent = ? I battery = ? V 1 = ? I 1 = ? V 2 = ? I 2 = ? I 2 =? V 2 =?
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C V C V d c b a C R d c b a
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Magnet B Close is strong B Far is weak Magnet B IL B rotate I I I I
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Magnet B I I I VV
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N solenoid loops enclosed in the Amperian loop, each with current I. n is “loop density” N/L of solenoid. B IN Amperian loop L Ampere’s Law:
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R L B incident induced by B acts like battery. Current flowing through resistor is easily measured. induced External Inductance R L induced Oscillating voltage source causes oscillating B inside inductor. Oscillating B inside inductor induces voltage induced (back EMF). Back EMF makes inductor seem like a resistor to the voltage source. Self Inductance
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R L B incident An oscillating external B causes an induced voltage induced across the inductor. induced External Inductance R L induced Oscillating voltage source causes oscillating B inside inductor which induces a voltage induced across the inductor. Self Inductance
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R L Self Inductance:
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I I I DC Power Supply + - brushes Magnet B
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I NS S N
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I I a y z x {outward}
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y z x
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V(t) t VLVL VRVR VSVS
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t V?V? V?V? VRVR
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t VLVL VCVC VRVR
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t VCVC VRVR VSVS
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t V?V? VRVR V?V?
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t VLVL VCVC VRVR VSVS
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VLVL VCVC VRVR VSVS t
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R [ohm] C [farad] V source L [henry]
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V s (t) + - 0 V s (t)-V R (t) V s (t)-V R (t)-V C (t) V s (t)-V R (t)-V C (t)- V L (t)=0 +Q -Q VSVS VCVC + + + - - - VRVR VLVL I(t)
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t V(t)
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[V] [t]
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[V] [t]
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[V] [t]
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Pulses let through by the diode move speaker with frequency of desired audio wave. Quantum mechanical turn-on voltage of diode. Modulate Wave Transmitted by Diode to Speaker [V] 0
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ANT GND A B PRIMARY SOLENOID SECONDARY SOLENOID
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ANT GND A B PRIMARY SOLENOID SECONDARY SOLENOID secondary circuit L sec
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ANT GND A B PRIMARY SOLENOID SECONDARY SOLENOID secondary circuit L sec /2
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Diode A B TUNER EAR
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3,600 [Hz]
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envelope [Hz] carrier [Hz] RF Modulator RF out low in CH 2 CH 1 modulated
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envelope [Hz] carrier [Hz] RF Modulator RF out low in CH 2 CH 1 modulated
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CH 2 CH 1 modulated antenna ground
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I amplitude f drive f resonance I amplitude f drive f resonance AB
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9 V R 1 = 1 R 2 = 2 R 3 = 3 R 4 =4 I 4 =? V 4 =? I 1 =? V 1 =?I 2 =? V 2 =? I 3 =? V 3 =? I Battery =? R equivalent =?
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BATTERY + a b c d
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+ + A B Total charge +Q & -Q ++++++++++++++ +++++++++ +++++ +++++ +++++ --------- --------- --------- --------- (-Q/2) (+Q/4) (+Q/2)
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R1R1 VSVS S1S1 R2R2 C S2S2 R 1 = 1x10 6 [ ] R 2 = 1x10 5 [ ] C = 1x10 -5 [F] V s = 10 [V]
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Thumb shows direction of magnetic field. B Wrap fingers in direction of current. q If charge q is negative, reverse B-field direction.
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B I I Thumb shows direction of magnetic field.
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BATTERY + voltage “height” 1.5 [V] 0 [V]
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BATTERY + voltage “height” 1.5 [V] 0 [V]
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BATTERY voltage “height” 1.5 [V] 0 [V] voltage 1.5 [V] 0 [V] position on circuit abcda 1.5 [V] a b c d a d c b
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BATTERY + voltage “height” 1.5 [V] 0 [V] a b c d e voltage 1.5 [V] 0 [V] position on circuit abcdea
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1.5 [V] R BULB 1.5 [V] R BULB a b c d e
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BATTERY + voltage “height” 1.50 [V] 0 [V] a b c 0.75 [V]
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BATTERY + voltage “height” 1.50 [V] 0 [V] 0.75 [V]
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voltage 1.50 [V] 0 [V] position on circuit abc 0.75 [V] a
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V R Bulb abc V a b f d ce
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a voltage “height” 1.5 [V] 0 [V] BATTERY + b c dfe
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voltage 1.50 [V] 0 [V] position on circuit fdb 0.75 [V] ace f aa
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display settings + positive terminal for high current measurements (has large fuse) - negative terminal or “ground” + positive terminal
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Voltage V DC V R BATTERY +
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? amps BATTERY + ? amps mA BATTERY + mA AB
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Amperes mA A R BATTERY +
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Amperes mA A R BATTERY +
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Ohms ( ) R
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3 V a b c d BATTERY + + ab cd R Bulb 1.5 [V] 0 [V] 3.0 [V] 3 V a b c d BATTERY + + ab c d 1.5 [V] 0 [V] 3.0 [V]
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V amp =3 V 330 CH1CH2 red1 red2 bottom ground x-y mode
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30 V Ground 1000 V 2000 V 3000 V constant voltage - - - - - ground - - - - -- - - - - - - - -
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30 V Ground 1000 V 2000 V 3000 V constant voltage charge separation ground
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+ + + + + - - - - - - - + + + + + + + + + + - - - - - - - + + + + - - - - - - - + + evenly arranged clustered positive clustered negative
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Real Imaginary VRVR tt VLVL VCVC VSVS shift
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Real Imaginary VRVR VLVL VCVC
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Im{V(t)} Re{V(t)} Real Imaginary V0V0 tt V(t)=V 0 e i t rotates around the complex plane in time.
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Voltage time VLVL VCVC VRVR VSVS
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R [ohm] C [farad] V source L [henry] R [ohm] C [farad] V source L [henry] THEORYREALITY
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NS
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x AB CDE
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x [cm] 10 [V]86420 0246810
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x [cm] 1086420 [V] 0246810 A B
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N solenoid loops enclosed in the Amperian loop, each with current I. n is “loop density” N/L of solenoid. B IN Amperian loop L Ampere’s Law:
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