1. CP2 Circuit Theory Dr Todd Huffman t.huffman1@physics.ox.ac.uk http://www-pnp.physics.ox.ac.uk/~huffman/ Aims of this course: Understand basic circuit components (resistors, capacitors, inductors, voltage and current sources, op-amps) Analyse and design simple linear circuits + – + +

2. Circuit Theory: Synopsis Basics: voltage, current, Ohm’s law… Kirchoff’s laws: mesh currents, node voltages… Thevenin and Norton’s theorem: ideal voltage and current sources… Capacitors: Inductors: AC theory: complex notation, phasor diagrams, RC, RL, LCR circuits, resonance, bridges… Op amps: ideal operational amplifier circuits… Op-amps are now on the exam syllabus Stored energy, RC and RL transient circuits

3. Reading List Electronics: Circuits, Amplifiers and Gates, D V Bugg, Taylor and Francis Chapters 1-7 Basic Electronics for Scientists and Engineers, D L Eggleston, CUP Chapters 1,2,6 Electromagnetism Principles and Applications, Lorrain and Corson, Freeman Chapters 5,16,17,18 Practical Course Electronics Manual http://www-teaching.physics.ox.ac.uk/practical_course/ElManToc.html Chapters 1-3 Elementary Linear Circuit Analysis, L S Bobrow, HRW Chapters 1-6 The Art of Electronics, Horowitz and Hill, CUP

4. Why study circuit theory? Foundations of electronics: analogue circuits, digital circuits, computing, communications… Scientific instruments: readout, measurement, data acquisition… Physics of electrical circuits, electromagnetism, transmission lines, particle accelerators, thunderstorms… Not just electrical systems, also thermal, pneumatic, hydraulic circuits, control theory

5. Mathematics required Differential equations Complex numbers Linear equations V(t)=V 0 e jωt V 0 –I 1 R 1 –(I 1 –I 2 )R 3 = 0 (I 1 –I 2 )R 3 –I 2 R 2 +2 = 0 Covered by Complex Nos & ODEs / Vectors & Matrices lectures

6. Charge, voltage, current Potential difference: V=V A –V B Energy to move unit charge from A to B in electric field Charge: determines strength of electromagnetic force quantised: e=1.62×10 -19 C [coulombs] [volts]

7. Power: rate of change of work No. electrons/unit vol Cross-section area of conductor Drift velocity Charge Q=e Current: rate of flow of charge [amps] [watts]

8. Ohm’s law Voltage difference  current I L A V R=Resistance Ω[ohms] ρ=Resistivity Ωm Resistor symbols: R

9. Resistivities Silver1.6×10 -8 Ωm Copper1.7×10 -8 Ωm Manganin42×10 -8 Ωm Distilled water5.0×10 3 Ωm PTFE~10 19 Ωm Conductance [seimens] conductivity [seimens/m] Power dissipation by resistor:

10. Voltage source V0V0 Ideal voltage source: supplies V 0 independent of current V0V0 R int Real voltage source: V load =V 0 –IR int R load +–+– battery cell

11. Constant current source Ideal current source: supplies I 0 amps independent of voltage Real current source: R load I0I0 R int I0I0 Symbol: or

12. AC and DC DC (Direct Current): Constant voltage or current Time independent V=V 0 AC (Alternating Current): Time dependent Periodic I(t)=I 0 sin(ωt) 50Hz power, audio, radio… +–+– + -

13. RMS values AC Power dissipation Why ? Square root of mean of V(t) 2

14. Passive Sign Convention Passive devices ONLY - Learn it; Live it; Love it! R=Resistance Ω[ohms] Which way does the current flow, left or right? Two seemingly Simple questions: Voltage has a ‘+’ side and a ‘-’ side (you can see it on a battery) on which side should we put the ‘+’? On the left or the right? Given V=IR, does it matter which sides for V or which direction for I?

15. Kirchoff’s Laws I Kirchoff’s current law: Sum of all currents at a node is zero I1I1 I3I3 I2I2 I4I4 I 1 +I 2 –I 3 –I 4 =0 (conservation of charge) Here is a cute trick: It does not matter whether you pick “entering” or “leaving” currents as positive. BUT keep the same convention for all currents on one node!

16. II Kirchoff’s voltage law:Around a closed loop the net change of potential is zero (Conservation of Energy) V0V0 I R1R1 R2R2 R3R3 5V 3kΩ 4kΩ Calculate the voltage across R 2 1kΩ

17. Kirchoff’s voltage law: V0V0 I 1k 3k 4k -V 0 +IR 1 +IR 2 +IR 3 =0 + + + + – – – – –V 0 +IR 1 +IR 2 +IR 1 5V=I(1+3+4)kΩ V R2 =0.625mA×3kΩ=1.9V

18. Series / parallel circuits R1R1 R2R2 R3R3 Resistors in series: R Total =R 1 +R 2 +R 3 … R1R1 R2R2 R3R3 Resistors in parallel Two parallel resistors:

19. Potential divider R1R1 R2R2 V0V0 USE PASSIVE SIGN CONVENTION!!! Show on blackboard

20. Mesh currents 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 I1I1 I2I2 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ Second job: USE PASSIVE SIGN CONVENTION!!! First job: Label loop currents in all interior loops + + + Third job: Apply KCL to elements that share loop currents Define: Currents Entering Node are positive I 1 –I 2 –I 3 = 0  I 3 = I 1 -I 2

21. Mesh currents 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 I1I1 I2I2 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ Last job: USE Ohm’s law and solve equations. Fourth job: Apply Kirchoff’s Voltage law around each loop. + + +

22. Mesh currents 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 I1I1 I2I2 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ -9V+I 1 R 1 +I 3 R 3 = 0 I 3 =I 1 –I 2 –I 3 R 3 +I 2 R 2 +2V = 0 9V/k Ω = 9I 1 –6I 2 -2V/kΩ = -6I 1 +8I 2  I 2 =1 mA + + + Solve simultaneous equations

23. Node voltages 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ VXVX 0V - - + - Step 1: Choose a ground node! Step 2: Label voltages on all unlabled nodes Step 3: Apply KCL and ohms law using the tricks

24. Node voltages 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ VXVX 0V USE PASSIVE SIGN CONVENTION!!! - - + - Only one equation, Mesh analysis would give two. All currents leave all labeled nodes And apply V/R to each current.

25. 2V 9V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 VXVX 0V

26. Thevenin’s theorem V eq R eq Any linear network of voltage/current sources and resistors  Equivalent circuit

27. In Practice, to find V eq, R eq … R L  (open circuit) I L 0 V eq =V OS R L 0 (short circuit) V L 0 V0V0 + R1R1 RLRL I1I1 I ss R2R2 I2I2 VLVL R2R2 I2I2 R eq = resistance between terminals when all voltages sources shorted – Warning! This is not always obvious!

28. Norton’s theorem R eq Any linear network of voltage/current sources and resistors  Equivalent circuit I0I0

29. V0V0 R1R1 R eq R load V L =V 0 –I L R 1 V0V0 R R 

30. using Thevenin’s theorem: from Prev. Already know V AB =V eq = 2V 2V + + R 1 =3kΩR 2 =2kΩ R 3 = 6kΩ A B 9V 2V + + A B R 2 =2kΩ + A B 2V 1kΩ I ss I1I1 I2I2

31. using Norton’s theorem: 2V + + R 1 =3kΩR 2 =2kΩ R 3 = 6kΩ A B 9V 1kΩ 2mA A B Same procedure: Find I SS and V OC I EQ = I SS and R EQ = V OC /I SS

32. Superposition 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 9V + R1R1 R2R2 R3R3 IAIA IBIB ICIC 2V + R1R1 R2R2 R3R3 IEIE IFIF IGIG = + I 1 =I A +I E I 2 =I B +I F I 3 =I C +I G Important: label Everything the same directions!

33. 9V + R1R1 R2R2 R3R3 IAIA IBIB ICIC + R1R1 R2R2 R3R3 IAIA IBIB ICIC R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ Example: Superposition

34. 2V + R1R1 R2R2 R3R3 IEIE IFIF IGIG + R2R2 R3R3 IFIF IEIE IGIG R1R1 R 1 =3kΩ R 2 =2kΩ R 3 =6kΩ

35. 9V 2V + + R1R1 R2R2 R3R3 I1I1 I2I2 I3I3 9V + R1R1 R2R2 R3R3 IAIA IBIB ICIC 2V + R1R1 R2R2 R3R3 IEIE IFIF IGIG = + I 1 =I A +I E I 2 =I B +I F I 3 =I C +I G

36. Matching: maximum power transfer V0V0 R in R load Find R L to give maximum power in load Maximum power transfer when R L =R in Note – power dissipated half in R L and half in R in

37. Circuits have Consequences Problem: –My old speakers are 60W speakers. –Special 2-4-1 deal at El- Cheap-0 Acoustics on 120W speakers!! (“Offer not seen on TV!”) –Do I buy them? Depends! 4 , 8 , or 16  speakers? Why does this matter?

38. And Now for Something Completely Different