Lesson 6 Direct Current Circuits Electro Motive Force

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Lesson 6 Direct Current Circuits ¨Electro Motive Force ¨Internal Resistance Lesson 6 ¨Resistors in

Lesson 6 Direct Current Circuits ¨Electro Motive Force ¨Internal Resistance Lesson 6 ¨Resistors in Series and Parallel ¨Kirchoffs Rules

Topics ·RC Circuits ·Charging ·Discharging Capacitors ·Electrical Instruments ·Galvanometer ·Ammeter ·Voltmeter ·Wheatstone Bridge ·Potentiometer

Topics ·RC Circuits ·Charging ·Discharging Capacitors ·Electrical Instruments ·Galvanometer ·Ammeter ·Voltmeter ·Wheatstone Bridge ·Potentiometer

Electro Motive Force (emf) EMF I Source of emf is any device that increases

Electro Motive Force (emf) EMF I Source of emf is any device that increases the potential energy of charges circulating in a circuit. Electric Potential increases by the emf E as charge goes from negative to positive plate of battery.

EMF II EMF is Work Done per unit charge by electrical pump e d.

EMF II EMF is Work Done per unit charge by electrical pump e d. W = d. Q

¨Battery is a Charge Pump ¨Current flowing internally in battery feels a resistance this

¨Battery is a Charge Pump ¨Current flowing internally in battery feels a resistance this is an ¨Internal resistance, r ¨Flowing positive charges (current) experience drop of electric potential in resistor V=IR + R - Charge Pump

Internal Resistance - - + + - + Terminals ¨Terminal Potential Difference ¨V =

Internal Resistance - - + + - + Terminals ¨Terminal Potential Difference ¨V = E - Ir

Picture

Picture

Power and Internal Resistance

Power and Internal Resistance

Combinations of Combination of Resistors ¨Parallel ¨same electric potential felt by each element ¨Series

Combinations of Combination of Resistors ¨Parallel ¨same electric potential felt by each element ¨Series ¨electric potential felt by the combination is the sum of the potentials across each element

Series

Series

Parallel

Parallel

Kirchoff’s Rules The sum of the currents entering a junction must equal the sum

Kirchoff’s Rules The sum of the currents entering a junction must equal the sum of the currents leaving Conservation of Charge Kirchoffs Rules I

Kirchoffs Rules II The Sum of the Potential Differences around a closed circuit loop

Kirchoffs Rules II The Sum of the Potential Differences around a closed circuit loop must be zero Conservation of Energy

Picture

Picture

RC Circuits ¨Non Steady State ¨Non Equilibrium ¨Current varies with time RC circuits

RC Circuits ¨Non Steady State ¨Non Equilibrium ¨Current varies with time RC circuits

Picture

Picture

Charging I

Charging I

e d dt æ ç è e - IR Þ - IR - q

e d dt æ ç è e - IR Þ - IR - q C = 0 ö q d. I ÷ = 0 - R C ø dt d. I I Û R + = 0 dt C d. I 1 Þ = dt I RC Charging II ò ò I d. I I = - 1 RC I 0 Þ - 1 C dq dt t dt 0 æ I ö t ÷ = ln ç è I 0 ø RC I(t ) = I (t) = I 0 e Û e R e - t RC

e I (t ) = e R Charging III e dq - dt =

e I (t ) = e R Charging III e dq - dt = R e Þ dq = ò q dq = R Þ q (t ) = C e R e e ò e 0 é ê 1 êë e - t RC - t RC dt t e - t RC dt 0 ù é ú = Q ê 1 úû êë e - t RC ù ú úû

Time Constant

Time Constant

Discharging I +Q -Q IR = q from Kirchoff C dq = I dt

Discharging I +Q -Q IR = q from Kirchoff C dq = I dt the rate of decrease of charge

Discharging II

Discharging II