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Lecture #6 methods of solving circuits

Lecture #6 methods of solving circuits. Nodal analysis Graphical analysis In the next lecture we will look at circuits which include capacitors In the following lecture, we will start exploring semiconductor materials (chapter 2). Reading: Malvino chapter 2 (semiconductors).

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Lecture #6 methods of solving circuits

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  1. Lecture #6 methods of solving circuits • Nodal analysis • Graphical analysis • In the next lecture we will look at circuits which include capacitors • In the following lecture, we will start exploring semiconductor materials (chapter 2). • Reading: Malvino chapter 2 (semiconductors) EE 42 fall 2004 lecture 6

  2. Nodal analysis • So far, we have been applying KVL and KCL “as needed” to find voltages and currents in a circuit. • Good for developing intuition, finding things quickly… • …but what if the circuit is complicated? What if you get stuck? • Systematic way to find all voltages in a circuit by repeatedly applying KCL: node voltage method EE 42 fall 2004 lecture 6

  3. Branches and Nodes Branch: elements connected end-to-end, nothing coming off in between (in series) Node: place where elements are joined—includes entire wire EE 42 fall 2004 lecture 6

  4. a b + + + Vb Va _ _ _ ground Node Voltages The voltage drop from node X to a reference node (ground) is called the node voltage Vx. Example: EE 42 fall 2004 lecture 6

  5. Nodal Analysis Method 1. Choose a reference node (aka ground, node 0) (look for the one with the most connections, or at the bottom of the circuit diagram) 2. Define unknown node voltages (those not connected to ground by voltage sources). 3. Write KCL equation at each unknown node. • How? Each current involved in the KCL equation will either come from a current source (giving you the current value) or through a device like a resistor. • If the current comes through a device, relate the current to the node voltages using I-V relationship (like Ohm’s law). 4. Solve the set of equations (N linear KCL equations for N unknown node voltages). EE 42 fall 2004 lecture 6 * with “floating voltages” we will use a modified Step 3

  6. V b R 3 R 4 Example What if we used different ref node? node voltage set  R1 Va • Choose a reference node. • Define the node voltages (except reference node and the one set by the voltage source). • Apply KCL at the nodes with unknown voltage. • Solve for Va and Vb in terms of circuit parameters. + IS V1 R - 2  reference node EE 42 fall 2004 lecture 6

  7. Example R 1 Va R 5 R I 3 1 V V R R 2 1 2 4 EE 42 fall 2004 lecture 6

  8. Load line method • I-V graph of circuits or sub-circuits • I-V graph of non-linear elements • Using I-V graphs to solve for circuit voltage, current (The load-line method) • Reminder about power calculations with nonlinear elements. EE 42 fall 2004 lecture 6

  9. (ma) I 1K + - + - 4 Combined 1K + 4K V1 V I + - V2 2 4K V (Volt) 5 Example of I-V Graphs Resistors in Series If two resistors are in series the current is the same; clearly the total voltage will be the sum of the two IR values i.e. I(R1+R2). Thus the equivalent resistance is R1+R2 and the I-V graph of the series pair is the same as that of the equivalent resistance. Of course we can also find the I-V graph of the combination by adding the voltages directly on the I-V axes. Lets do an example for 1K + 4K resistors 1K 4K EE 42 fall 2004 lecture 6

  10. (ma) I Combined 2K + 2V 2V + - 2V + - 4 V I 2K 2K 2 V (Volt) I 5 Example of I-V Graphs Simple Circuit, e.g. voltage source + resistor. If two circuit elements are in series the current is the same; clearly the total voltage will be the sum of the voltages i.e. VS + IR. We can graph this on the I-V plane. We find the I-V graph of the combination by adding the voltages VS and I R at each current I. Lets do an example for =2V, R=2K VS EE 42 fall 2004 lecture 6

  11. (A) I I=0.85A at 117V + - 0.8 V I 0.4 V (Volt) 100 Example of I-V Graphs Nonlinear element, e.g. lightbulb If we think of the light bulb as a sort of resistor, then the resistance changes with current because the filament heats up. The current is reduced (sort of like the resistance increasing). I say “sort of” because a resistor has, by definition a linear I-V graph and R is always the same. But for a light bulb the graph kind of “rolls over”, becoming almost flat. Consider a 100 Watt bulb, which means at at the nominal line voltage of 117 V the current is 0.85A. (117 V times 0.85 A = 100W). EE 42 fall 2004 lecture 6

  12. (ma) I 2.5V I Solution: I = 0.5mA, V = 2.5V 4 1K + - + - Combined 1K + 4K 2.5V V 4K 2 V (Volt) 5 I-V Graphs as a method to solve circuits We can find the currents and voltages in a simple circuit graphically. For example if we apply a voltage of 2.5V to the two resistors of our earlier example: We draw the I-V of the voltage and the I-V graph of the two resistors on the same axes. Can you guess where the solution is? At the point where the voltages of the two graphs AND the currents are equal. (Because, after all, the currents are equal, as are the voltages.) This is called the LOAD LINE method; it works for harder (non-linear) problems. EE 42 fall 2004 lecture 6

  13. I (ma) I + - Solution: I = 0.7mA, V = 1.4V 2V 4 V 2K 2 V (Volt) 5 Another Example of the Load-Line Method Lets hook our 2K resistor + 2V source circuit up to an LED (light-emitting diode), which is a very nonlinear element with the IV graph shown below. Again we draw the I-V graph of the 2V/2K circuit on the same axes as the graph of the LED. Note that we have to get the sign of the voltage and current correct!! (The sing of the current is reversed from page 3) At the point where the two graphs intersect, the voltages and the currents are equal, in other words we have the solution. LED + - LED EE 42 fall 2004 lecture 6

  14. Power of Load-Line Method We have a circuit containing a two-terminal non-linear element “NLE”, and some linear components. The entire linear part of the circuit can be replaced by an equivalent, for example the Thevenin equivalent. This equivalent circuit consists of a voltage source in series with a resistor. (Just like the example we just worked!). So if we replace the entire linear part of the circuit by its Thevenin equivalent our new circuit consists of (1) a non-linear element, and (2) a simple resistor and voltage source in series. If we are happy with the accuracy of graphical solutions, then we just graph the I vs V of the NLE and the I vs V of the resistor plus voltage source on the same axes. The intersection of the two graphs is the solution. (Just like the problem on page 6) EE 42 fall 2004 lecture 6

  15. 200K +- 2V ID D D Non-linear element NLE 1M + - 250K VDS 9mA +- S S The Load-Line Method We have a circuit containing a two-terminal non-linear element “NLE”, and some linear components. First replace the entire linear part of the circuit by its Thevenin equivalent (which is a resistor in series with a voltage source). We will learn how to do this in Lecture 11. Then define I and V at the NLE terminals (typically associated signs) 1V NOTE: In lecture 11 we will show that the circuit shown on the left is equivalent to a 200K resistor in series with 2V. EE 42 fall 2004 lecture 6

  16. ID D 200K 200K +- +- 2V 2V S ID ID (mA) D 10 NLE + - The solution ! VDS + - VDS S VDS (V) 1 2 Example of Load-Line method (con’t) Given the graphical properties of two terminal non-linear circuit (i.e. the graph of a two terminal device) And have this connected to a linear (Thévenin) circuit Whose I-V can also be graphed on the same axes (“load line”) The intersection gives circuit solution EE 42 fall 2004 lecture 6

  17. ID D 200K +- 2V S ID (mA) 10 The solution ! VDS (V) 1 2 Load-Line method The method is graphical, and therefore approximate But if we use equations instead of graphs, it could be accurate It can also be use to find solutions to circuits with three terminal nonlinear devices (like transistors), which we will do in a later lecture EE 42 fall 2004 lecture 6

  18. Power Calculation Review Power is calculated the same way for linear and non-linear elements and circuits. For any circuit or element the dc power is I X V and, if associated signs are used, represents heating for positive power or extraction of energy for negative signs. For example in the last example the NLE has a power of +1V X 5mA or 5mW . It is absorbing power. The rest of the circuit has a power of - 1V X 5mA or - 5mW. It is delivering the 5mW to the NLE. So what it the power absorbed by the 200K resistor? Answer: I X V is + 5mA X (5mA X 200K) = 5mW. Then the voltage source must be supplying a total of 10mW. Can you show this? EE 42 fall 2004 lecture 6

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