ELEC1130 Lecture 110 2016/17 Quiz School of Electronic and Electrical Engineering Is the diode on the right forward biassed or reverse biassed? Will current flow or not? ELEC 1130 Lecture 110 –ve on left, +ve on right – + Diodes (2) 2016/17 ELEC 1130 Dr C. Trayner Quiz Summary When a normal Si diode is conducting, what is the approximate voltage lost across it? 1. 0 V 2. 0.7 V 3. 5 V 4. 230 V Last time: • Introduction to diodes • Voltage and current sources 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 2 Today: • More details of diodes • Understanding last week’s lab and preparing for this week’s 3 2016/17 ELEC 1130 Dr C. Trayner 4 1 ELEC1130 Lecture 110 2016/17 Terminology - revision Ways of thinking of the ideal diode - revision Names of electrodes Forward biassed current will flow Anode Cathode + + – Reverse biassed current will not flow Circuit symbol Triangle may be filled in or empty as you prefer 2016/17 Forward biassed – – 5 I/V curve of the ideal diode + 2016/17 Dr Chris Trayner = 2016/17 Open circuit = ELEC 1130 Dr C. Trayner Open switch = 6 What did you find in the lab? What sort of I/V curve did you get? • Straight? • Curving upwards? • Curving downwards? Forward bias: no voltage drop whatever the current Reverse bias: no current whatever the voltage ∞Ω The real diode I V – + = = = Reverse biassed + ELEC 1130 Dr C. Trayner – Closed switch Short circuit 0Ω + – ELEC 1130 Dr C. Trayner 7 2016/17 ELEC 1130 Dr C. Trayner 8 2 ELEC1130 Lecture 110 2016/17 The real diode ELEC 1130 Dr C. Trayner 9 Do diodes obey Ohm’s Law? Ohm’s law is not always true But for most electronic components 2016/17 ELEC 1130 Dr C. Trayner The real diode – a surprisingly simple approximation Voltage ELEC 1130 Dr C. Trayner 11 2016/17 ELEC 1130 Dr C. Trayner Figure: Dr H. Eisele ~0.7 V Tangent over short section Dr Chris Trayner 10 Current • it is true • or at least to a good enough approximation • or it is approximately true under limited conditions For diodes the third case is occasionally useful 2016/17 Figure: Dr H. Eisele Figure: Dr H. Eisele 2016/17 Resistors are simple to model i.e. to calculate with Diodes are more complicated but we would still like a simple model – even if an approximation 12 3 ELEC1130 Lecture 110 2016/17 How do we model this? What if this approximation isn’t good enough? What equivalent circuit can we have for the rule of thumb of 0.7 V? An ideal diode in series with a 0.7 V ideal source 2016/17 ELEC 1130 Dr C. Trayner 13 Another fairly simple approximation 0.7 V 2016/17 Figure: Dr H. Eisele Figure: Dr H. Eisele (Rb is the currentlimiting resistor) ELEC 1130 Dr C. Trayner 14 How do we model this? Diode simulated by a voltage source and an internal resistance Straight but sloping line Behaves like a resistor but for the offset Figure: Dr H. Eisele < 0.7 V And an ideal diode (here shown forward biassed) Figure: Dr H. Eisele 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 15 2016/17 ELEC 1130 Dr C. Trayner 16 4 ELEC1130 Lecture 110 2016/17 So we have four models Another fairly simple approximation It looks scary but try analysing it Ideal diode This is of the form exp(kV) k is a horizontal scaling factor Actually quite large 0.7 V <0.7 V & Rs Exact equation Figure: Dr H. Eisele 2016/17 ELEC 1130 Dr C. Trayner Except for tiny or –ve V, this is smaller than exp(kV) and can be ignored This is just a vertical scaling factor Actually very small 17 2016/17 ELEC 1130 Dr C. Trayner Exponentials – mysterious? Exponentials – mysterious? Consider ex (also written exp(x) ) e is just a number (about 2.718) Compare with other examples of kx 2x: 1, 2, 4, 8, 16, … 10x: 1, 10, 100, 1000, 10000, ... These grow fast, the curve gets steeper These are the same sort of curve The k in kx is just a horizontal scaling factor They can be continued the other way for –ve x: 2x: 1/16, 1/8, 1/4, 1/2, 1, 2, 4, 8, 16, … 10x: 0.0001, 0.001, 0.01, 0.1, 1, 10, 100, 1000, 10000, ... As x gets more and more –ve, kx tends asymptotically towards zero 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 19 2016/17 ELEC 1130 Dr C. Trayner 18 20 5 ELEC1130 Lecture 110 2016/17 exp(x) exp(x) and exp(x)–1 2016/17 ELEC 1130 Dr C. Trayner 21 So we have four models 2016/17 ELEC 1130 Dr C. Trayner 22 So we have four models When should you use which model? Common sense should tell you • Is the 0.7 V significant compared with the voltages it will be handling? • How much precision do you need? Ideal diode 0.7 V <0.7 V & Rs Exact equation Figure: Dr H. Eisele 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 23 2016/17 ELEC 1130 Dr C. Trayner 24 6 ELEC1130 Lecture 110 2016/17 What can you do with diodes? The half-wave rectifier Power supplies: PSUs, battery chargers, … Mains is • nominally sine wave (waveform may be a bit rough), • 50 Hz or 60 Hz in some parts of the world • typically around 230 V RMS This needs to be reduced to low voltages and turned from AC to DC AC provided by transformer Load receives DC (would normally be smoothed) 2016/17 ELEC 1130 Dr C. Trayner Figure: Dr H. Eisele Transformers reduce the voltage • more complicated with switched-mode PSUs Diodes are part of the AC to DC conversion 25 2016/17 ELEC 1130 Dr C. Trayner The full-wave rectifier bridge Only uses the +ve half cycles Four diodes (the bridge) Two conduct at any time • two for +ve half cycle • two for –ve half cycle 50% of the time is wasted 2016/17 Dr Chris Trayner Figure: Dr H. Eisele (actually a bit more with non-ideal diodes) ELEC 1130 Dr C. Trayner 27 2016/17 Figure: Dr H. Eisele The half-wave rectifier 26 ELEC 1130 Dr C. Trayner 28 7 ELEC1130 Lecture 110 2016/17 +ve half cycle Follow the current route Convince yourself that • the red diodes are forwardbiassed • the black ones are reversebiassed • current flows downwards through the load –ve half cycle Follow the current route Convince yourself that • the red diodes are forwardbiassed • the black ones are reversebiassed • current flows downwards through the load 2016/17 ELEC 1130 Dr C. Trayner 29 2016/17 Figure: Dr H. Eisele The full-wave rectifier bridge Figure: Dr H. Eisele The full-wave rectifier bridge ELEC 1130 Dr C. Trayner Half-wave vs full-wave Rectifying and smoothing Which is the more economical (for a given average current)? Discuss Diodes only change from AC to DC Leaves a very variable voltage Needs smoothing One capacitor will smooth it somewhat 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 31 2016/17 ELEC 1130 Dr C. Trayner 30 32 8 ELEC1130 Lecture 110 2016/17 Real power supplies Traditionally you add a second capacitor (with a resistor in between the two) • This gave moderate smoothing with fairly large capacitors • but voltage dropped as loading current increased 2016/17 Figure: Dr H. Eisele Still somewhat rough ELEC 1130 Dr C. Trayner 33 Modern approach is a regulator chip • only needs one capacitor • keeps the voltage fixed • also sets a current limit 2016/17 ELEC 1130 Dr C. Trayner Online homework: google for a data sheet for a 78XX IC, e.g. 7805 for 5 V 34 Summary Diodes: • one-way valves for current • ideal and real diodes • approximations to real diodes • and the equation 2016/17 Dr Chris Trayner ELEC 1130 Dr C. Trayner 35 9