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The Lead Acid Electric Battery I Sulfuric Acid Electrolyte: - Terminals + Sulfuric Acid Solution H2SO4 Spongy Lead (Pb) Lead Oxide (PbO2) Cell: 2 V Battery: Multiple cells H 2SO 4 2H 2O 2H 3O SO 42 Oxidation at the Negative Plate (Electrode:Anode): Pb SO42 PbSO4 2e Reduction at the Positive Plate (Electrode:Cathode): PbO2 4H3O SO42 2e PbSO4 6H 2 O Batteries Vab Ir Electromotive Force r Batterey internal resistance Kirchoff’s Rules • Conservation of charge • Junction (Node) Rule: At any junction point, the sum of all currents entering the junction must equal the sum of the currents leaving the junction. • Conservation of energy • Loop Rule: The some of the changes in potential around any closed path of a circuit must be zero. Energy in a circuit Series Circuit Apply the Loop Rule Vac Vab Vbc 0 + Vac Vac Vab Vbc IR1 IR 2 I R1 R 2 IR eq R eq R1 R 2 ..... Parallel Circuits I I1 I3 + Apply the Junction Rule I2 V 1 V V V 1 1 V I I1 I2 I3 V R1 R 2 R 3 R1 R 2 R 3 R eq 1 1 1 1 .... R eq R1 R 2 R 3 Rule Set – Problem Solving Strategy • A resistor transversed in the direction of assumed current is a negative voltage (potential drop) • A resistors transversed in the opposite direction of assumed current is a positive voltage (potential rise) • A battery transversed from – to + is a positive voltage. • A battery transversed from + to - is a negative voltage. • Ohm’s Law applies for resistors. • Both the loop rule and junction rule are normally required to solve problems. More about the Loop Rule • Traveling around the loop from a to b • In (a), the resistor is traversed in the direction of the current, the potential across the resistor is – IR • In (b), the resistor is traversed in the direction opposite of the current, the potential across the resistor is is + IR Loop Rule, final • In (c), the source of emf is traversed in the direction of the emf (from – to +), and the change in the electric potential is +ε • In (d), the source of emf is traversed in the direction opposite of the emf (from + to -), and the change in the electric potential is -ε Example Problem 1 Given: R1 1690 R 3 1000 R 4 3000 V = 3 Volts Find: current in each resistor Example Problem 2 Given: 10V 5 10 20 20V Find: current in the 20 resistor Alternating Current V t Vo I t Io V t Vo sin t V t Vo I(t) sin t Io sin t R R AC Power P I2R I2o R sin 2 t 1 2 1 Vo2 P Io R 2 2 R T/2 1 1 2 sin t dt ? T T / 2 2 Root Mean Square (rms) V t Vo sin t I(t) Io sin t 2 V V2 o 2 Vrms 2 I I2 o 2 2 V Vo 2 o V 2 2 I rms 1 2 2 P Io R I rms R 2 2 1 Vo2 Vrms P 2 R R 2 I Io 2 o I 2 2 The Wheatstone bridge a simple Ohmmeter I3R 3 I1R1 I3R x I1R 2 R2 Rx R3 R1 Charging a capacitor in an RC circuit Same Symbol At t = 0, Qo = 0 and I o R Solving the charging differential equation Kirchoff’s loop rule Q IR 0 C Convert to a simple equation in Current by taking the first derivative w.r.t. time dI 1 dQ R 0 dt C dt dI 1 R I dt C Separate variables dI 1 dt I RC Integrate the results I t Io t dI 1 dt I RC 0 t ln I t ln I o RC It t ln RC Io t It e RC Io I t Io e t RC Charge buildup dQ It Io e dt dQ Io e Q t 0 t RC t dQ Io e t RC dt t RC dt 0 Q t Io RC e t RC t t RC I RC 1 e o 0 Discharging the capacitor in an RC circuit At t = 0, Q = Qo Solving the discharging differential equation Q IR 0 C dQ 1 R Q dt C dQ 1 dt Q RC Kirchoff’s loop rule dQ I since charge is decreasing dt Separate variables Q t Integrate Qo t dQ 1 dt Q RC 0 Charge and current decay t ln Q t ln Qo RC Qt t ln RC Qo t Qt e RC Qo Q t Qo e t RC Charge and current decay dQ d I Qo e dt dt Qo RCt I e RC I Io e t RC t RC Electrical Safety • Current kills, not voltage (70 mA) • Normal body resistance = 105 But could be less than 1000 • Take advantage of insulators, remove conductors • Work with one hand at a time • Shipboard is more dangerous • Electrical safety is an officer responsibility