PH104 w/Dr G Lec 25 (filled) ELECTRIC CURRENT (Ch. 23) Can you imagine life without electricity? PH 104 w/ dr. g Lec 25 Charged objects: Spark = an electric current Spark jumping air gap with charged object: Electrons attracted across the gap, but air is insulator When charge high enough, air becomes temporary conductor Temporary CHARGE FLOW = “CURRENT” through air Electrons hop from one atom to next, bucket-brigade style When (-) ion gives up excess electron to next atom: energy released! After spark, less charge imbalance 1 2 How to sustain current through a conductor: Current in a spark: electrons “pulled” -through the air - - - Away from negative, and/or towards High e/c High p.e. positive, OR: From higher to lower electric potential energy Field: each point has “potential” = energy/charge (voltage) Electric current flows from higher Low e/c Low p.e. voltage to lower voltage + + + + + + + OR: charges “fall down” a voltage difference Voltage difference across a conductor: Electrons relatively free to move around Charges will flow from high voltage to low voltage: conductor) current From (+) voltage to (-) voltage (+ end to – end of Voltage drop ‐ + Charged objects: Spark = an electric current – 3 4 How to sustain current through a conductor: Sustained current (direct current or DC): Voltage difference must be maintained : Battery: “re-cycles” charges through conductor outside Voltage difference = J/C or lost by charges, to conductor 1 Volt = energy equal to 1 Joule per Coulomb 12-V: maintains voltage difference of 12 V across the conductor Inside battery: Each coulomb of charge given 12 J of energy + How to sustain current through a conductor: Charges: after losing potential energy, must be “re-energized” in cycle Performs WORK on the lower-energy charges current Connect conductor across a BATTERY !! + Voltage drop Need: charge “pump” or “voltage source” High V Low V – – 5 6 1 PH104 w/Dr G Lec 25 (filled) D.C. through a conductor: Details D.C. through a conductor: Details Current = amount of charge flow per second Flowing past any point: Coulombs/sec = Amperes (A) In conductor (outside battery): from (+) terminal to (-) terminal Current ~ Voltage difference: I ~ V V Conductor details: + – I Materials: different RESISTANCE (R) to electric current SAME voltage across different R: get different current I = V / R (Definition of R) (or: V = I R) Units: I – amperes, A; V – volts, V; R – V/A = ohms (Ω) Power rating of circuit element: energy needed per sec J/sec = J/C x C/s = V x I (Volt-amps = WATTS) V + – I R 7 8 Electrical circuits: I pumped by V in loop thru R Electrical circuits: I pumped by V in loop thru R R: details: Usually: higher-R “resistor(s)” connected by low-R “leads” Series combination of R’s: connected in “train” from (+) to (-) Parallel combination of R’s: each R connect across terminals V is divided among R’s ; same I through each I is divided among R’s ; connected across same V Energy delivered to circuit: same across each R Adding R decreases resistance of combination (more choices) Energy delivered to circuit: shared among the R’s I1 Adding R increases resistance of combination I I – + V1 V2 + I2 – I1 + I2 + I3 = I I3 V3 V1 = V2 = V3 V = V1 + V2 + V3 9 10 2