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Reading Assignment: Chapter 2 in Electric Circuits, 9 th Edition by Nilsson

Chapter 2 EGR 271 – Circuit Theory I. 1. Reading Assignment: Chapter 2 in Electric Circuits, 9 th Edition by Nilsson . Chapter 2: Electrical Devices Several types of electrical devices are introduced in this chapter, including independent sources, dependent sources, and resistors.

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Reading Assignment: Chapter 2 in Electric Circuits, 9 th Edition by Nilsson

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  1. Chapter 2 EGR 271 – Circuit Theory I 1 Reading Assignment: Chapter 2 in Electric Circuits, 9th Edition by Nilsson Chapter 2: Electrical Devices Several types of electrical devices are introduced in this chapter, including independent sources, dependent sources, and resistors. Independent sources – 2 types: 1) Independent voltage source 2) Independent current source

  2. Chapter 2 EGR 271 – Circuit Theory I 2 Long bar represents positive terminal Battery General Sinusoidal Voltage Voltage Source Source (e.g., 10sin(120t) V) 2A 100A 20A Circuit 1 Circuit 3 Circuit 2 12V 12V 12V • Independent voltage source – a device which maintains its specified voltage for any load current that is required. • Symbols: • The symbols shown above are from PSPICE. The boxes on the ends of the wires are simply for connecting wires or other components to the sources. • Voltages sources have a specified voltage, but the current depends on the circuit and is determined through analysis. • Example: The current provided by the 12V source below varies in each case.

  3. Chapter 2 EGR 271 – Circuit Theory I 3 Independent voltage source characteristics The “characteristics” of a device typically refers to a graph of I versus V which illustrates the behavior of the device. The characteristics of an ideal independent 12 V voltage source are shown below. I Current can have any value (depends on the circuit) V 12V Voltage is fixed at 12V

  4. Chapter 2 EGR 271 – Circuit Theory I 4 • Real versus ideal independent voltage sources • The voltage delivered by an real voltage source (or practical voltage source) will typically drop as the current required by the source increases. For example: • The 1.5V across a D-cell in a flashlight drops when the light is turned on. • The 12V across a car battery drops when the car is started. • The voltage from a power company drops during peak load hours (the voltage typically ranges from 115V - 130V). • Example: I Ideal 12V voltage source Real 12V voltage source V 12V Note: Any voltage source shown in the text is assumed to be ideal.

  5. Chapter 2 EGR 271 – Circuit Theory I 5 + + + Circuit 2 Circuit 3 Circuit 1 75V 200V 10V 2A 2A 2A _ _ _ • Independent current source – a device which maintains its specified current for any load voltage that is required. (This device is not as common in everyday use as the independent voltage source.) • Symbol: • The symbol shown above is from PSPICE. The boxes on the ends of the wires are simply for connecting wires or other components to the source. • Current sources have a specified current, but the voltage depends on the circuit and is determined through analysis. • Example: The voltage provided by the 2A source below varies in each case.

  6. Chapter 2 EGR 271 – Circuit Theory I 6 I 2A Current is fixed at 2A V I Ideal 2A current source 2A Real 2A current source V Independent current source characteristics The characteristics of an ideal independent 2A current source are shown below. Voltage can have any value (depends on the circuit) Real versus ideal independent current sources The current delivered by an real current source (or practical current source) will typically drop as the voltage required by the source increases. Example: Note: Any current source shown in the text is assumed to be ideal.

  7. Chapter 2 EGR 271 – Circuit Theory I 7 A l Resistance – the ability of a material to resist the flow of charge through it. Resistance is related to the physical dimensions and resistivity of a material as follows: where l = length of conductor (in cm) A = cross-sectional area of conductor  = resistivity of the material (in cm) • Resistivity varies tremendously in materials and is related to the atomic structure of the material. • Low resistivity: Some elements have electrons which are easily broken free (such as those with a single electron in the outer shell) so charge can easily move through the material. • High resistivity: Some elements have electrons which are tightly held (such as with a full outer shell) so charge cannot easily move through the material.

  8. Chapter 2 EGR 271 – Circuit Theory I 8 • Materials are sometimes classified as follows: • Conductor – a material with low resistivity. Examples (at 20oC) : • Copper:  = 1.68 x 10-8 cm • Silver:  = 1.59 x 10-8 cm • Aluminum:  = 2.65 x 10-8 cm • Insulator – a material with high resistivity. Examples: • Mica:  = 1.0 x 10+12 cm • Quartz (fused):  = 7.5 x 10+17 cm • Semiconductor – a material with neither very high nor very low resistivity. Conductivity is controlled through “doping” of the material (adding other elements) and through application of voltages. Examples: • Silicon:  = 0.1 - 60 x 10-3 cm • Germanium:  = 1 - 500 x 10-3 cm Conductivity – The inverse of resistivity. Conductivity is a measure of how well a material allows the flow of charge through it. Conductivity =  = 1/ 

  9. Chapter 2 EGR 271 – Circuit Theory I 9 Resistor – A circuit element with some specified value of resistance. The following symbol is used for a resistor: Typical values: Most resistance value in circuits are in the range 1 - 10 M Example: Find the resistance of a 200 m length of #12 copper wire (radius = 0.105 cm).

  10. Chapter 2 EGR 271 – Circuit Theory I 10 _ + 75V I 2.7k Ohm’s Law: Georg Simon Ohm established that there is an algebraic relationship between voltage and current for a resistor. This is easily shown experimentally by varying the voltage across a resistor and measuring the current through it. V = IR (so 1 = 1V/A) Passive Sign Convention: A resistor is a passive device (it can only absorb energy) so Ohm’s Law must use passive sign convention. Example: Calculate the current through the resistor shown below.

  11. Chapter 2 EGR 271 – Circuit Theory I 11 I V Resistor Characteristics and Ohm’s Law Ohm’s Law is easily shown experimentally by varying the voltage across a resistor and measuring the current through it. The result is a plot of the “characteristics” for a resistor which show a linear relationship. Note that straight-line sections in I-V characteristics are often indicative of resistance. Examples: Sketch characteristics for a JFET (ohmic region), a light-bulb filament, or a tunnel diode.

  12. Chapter 2 EGR 271 – Circuit Theory I 12 Conductance: Conductance, G, is the inverse of resistance and is a measure of a device’s ability to allow the flow of charge through it. Resistance is used more commonly, but conductance is used on occasion.  Example: Calculate the conductance of a resistor with R = 2.7 k.

  13. Chapter 2 EGR 271 – Circuit Theory I 13 R R 1k 1k • Variable resistors: Two names are used for variable resistors: • potentiometer - Most common name (discuss other uses) • rheostat 15T Symbols 12T 12T 10T 1T 1T Examples: Pass around examples of potentiometers. ¾ turn (1T) and 15T turn potentiometers. Reference for images: www.jameco.com

  14. Chapter 2 EGR 271 – Circuit Theory I 14 Power absorbed by resistors: Resistors are passive devices and can only absorb power. Power can be calculated in three ways: Substituting Ohm’s Law into the equation above yields: Example: A 100W light bulb operates using 120V. Determine R and I for the bulb. Example:Determine Imax and Vmax for a 47 k, ¼ W resistor.

  15. Chapter 2 EGR 271 – Circuit Theory I 15 45mA 35mA R1 R2 330 150  ¼ W ½ W 1 W 2 W Power ratings for resistors: Resistors dissipate energy by giving off heat and/or light. Power ratings are related to the physical size of a resistor and to the type of material from which it is made. Carbon resistors are often color coded (with the value of resistance) and their size is related to their power rating. Example: An engineer designs a circuit with the values shown below. If the circuit is to be built in lab, what are the minimum power ratings that should be used for resistors R1 and R2? Demonstration – Pass around other types of resistors and discuss power ratings.

  16. Chapter 2 EGR 271 – Circuit Theory I 16 Examples of resistors: Carbon Resistors Ref: www.wikipedia.com Carbon Resistors Ref: www.wikipedia.com 7W Ceramic Resistor Ref: www.rapidonline.com Wirewound Resistor Ref: www.newark.com DIP Resistors Ref: www.jameco.com

  17. Chapter 2 EGR 271 – Circuit Theory I 17 Two key laws for analyzing circuits: Kirchhoff’s Voltage Law (KVL) Kirchhoff’s Current Law (KCL) Kirchhoff’s Voltage Law (KVL) Definition: “The algebraic sum of the voltages around any closed path equals zero.” Discuss. • Notes: • Start at any point in a path • Go around the loop in either direction until you return to the starting point • Use a consistent sign convention • Two possible sign conventions: • + to -  + term • - to +  - term • + to -  - term • - to +  + term • The first convention is most often used. • Hint: Use the sign that you hit first going around a loop.

  18. Chapter 2 EGR 271 – Circuit Theory I 18 _ _ + V2 + V4 _ _ + V1 V3 V5 + _ + Example: Use KVL around various closed paths. Sign convention: Use the sign that you hit first. KVL, left loop: -V1 +V2 - V3 = 0 (discuss) KVL, right loop: KVL, outer loop:

  19. Chapter 2 EGR 271 – Circuit Theory I 19 a 7V -9V 17V 13V -19V b _ + Vx 12V A + _ A VAB VBA _ B + B Example: Use KVL around the circuit below to find the voltage Vx. Discuss the difference in a sign due to convention and a sign due to the value of the voltage. Two-subscript notation: Generally the polarity must be indicated with a voltage for it to be clearly defined. Another way to specify the polarity is to add subscripts indicating the location of the positive and negative terminals. For example: VAB = the voltage from A to B with the positive terminal at A VBA = the voltage from A to B with the positive terminal at B ( Note that VAB = -VBA)

  20. Chapter 2 EGR 271 – Circuit Theory I 20 a 7V -9V 17V 13V -19V b _ + Vx 12V Example: Illustrate how two-subscript voltages are used with BJT’s. Label VCE, VBE, and VCB and use KVL to show a relationship between the voltages. Example: Use KVL to find Vabin the previous example. Recall that Vx = _____. Repeat using an alternate path for KVL.

  21. Chapter 2 EGR 271 – Circuit Theory I 21 Kirchhoff’s Voltage Law can be used to show an important law about parallel elements. Definitions for nodes and parallel elements are first introduced. Node: A node is a junction in a circuit where two or more elements have a common connection. Additionally, there can never be two nodes connected by a wire (this would form a single node). Note: Nodes are sometimes confused with connection points (or solder points). For example, the text typically uses solid circles (dots) to indicate connection points where three or more elements connect. These points may or may not be nodes. Node and a connection point Node, but not a connection point These two connection point are a single node

  22. Chapter 2 EGR 271 – Circuit Theory I 22 Example: How many nodes are in each circuit below? Label them.

  23. Chapter 2 EGR 271 – Circuit Theory I 23 Parallel Circuit Elements: Two circuit elements are “in parallel” if they share the same two nodes. Example: Identify the nodes and the parallel elements in the circuit below. Note: Parallel circuit elements do not always appear as parallel lines! Example: Identify the nodes and the parallel elements in the circuit below.

  24. Chapter 2 EGR 271 – Circuit Theory I 24 Use KVL to show that: Parallel circuit elements have the same voltage. Parallel circuit: Circuits consisting of only parallel circuit elements are referred to as parallel circuits. Note that the order of the elements is not important. Example: Draw an example of a parallel circuit. Example: Household circuits (on a single circuit breaker) are examples of parallel circuits. Draw an example of a household circuit.

  25. Chapter 2 EGR 271 – Circuit Theory I 25 Kirchhoff’s Current Law (KCL) Three possible definitions are listed below. The first is the most general. Definition: “The algebraic sum of the currents crossing any closed surface equals zero.” Discuss. Definition: “The algebraic sum of the currents entering and leaving a node equals zero.” Discuss. Definition: “The sum of the currents entering a node equals the sum of the currents leaving a node.” Discuss. Note: Think of a closed surface as a bubble. If the bubble collapses to a point, it could be a node. So applying KCL to a node is a special case and applying it to a closed surface is more general.

  26. Chapter 2 EGR 271 – Circuit Theory I 26 I6 I2 I4 B A C I5 I1 I3 D Example: Use KCL at various closed surfaces and nodes. Discuss using a sign convention. • Two possible sign conventions: • Out = +, In = - • Out = -, In = + • The first convention is most often used. Closed Surface #1 KCL, node A (out = +): +I1 – I2 + I6 = 0 KCL, node B (out = +): KCL, closed surface #1 (out = +):

  27. Chapter 2 EGR 271 – Circuit Theory I 27 7A -3A -9A 4 2 A + 12V - + 16V - Ix 11A Example: Apply KCL to node A in the circuit below. Discuss the difference in a sign due to convention and a sign due to the value of the current.

  28. Chapter 2 EGR 271 – Circuit Theory I 28 10A + - I1 There are times when the most general definition of KCL is the most powerful. Two examples are provided below. Example: Find the current I1 in the circuit shown below. Hint: draw a bubble that encompasses the right half of the circuit and apply KCL. Example: An IEEE standard states that all currents should be defined as entering a device. Label the currents IB, IC, and IE for the Bipolar Junction Transistor (BJT) and use KCL to find the relationship between the currents.

  29. Chapter 2 EGR 271 – Circuit Theory I 29 Series Elements - 2 elements are considered to be “in series” if they share one node and no other element is connected to that node. Use KCL to show that: Series circuit elements have the same current. Example: Draw an example of a series circuit.

  30. Chapter 2 EGR 271 – Circuit Theory I 30 Combining voltage sources Key point: Voltage sources add algebraically in series. Example: Example: Illustrate the well-known fact that flashlight batteries must be put in the flashlight with the correct polarity.

  31. Chapter 2 EGR 271 – Circuit Theory I 31 Combining voltage sources (continued) Key point: Voltage sources should not be placed in parallel (unless they have the same voltage). Example: This is an improper connection. What law is violated here? + _ + _ 12V 20V Practical exception: Voltage sources of the same value are sometimes placed in parallel to increase the total current capability. Illustrate how a tow truck might use two 12Vbatteries where each battery can deliver 600 CCA (cold cranking amps). What is the maximum current that the truck can deliver?

  32. Chapter 2 EGR 271 – Circuit Theory I 32 Combining current sources Key point: Current sources add algebraically in parallel. Example: Example:

  33. Chapter 2 EGR 271 – Circuit Theory I 33 Combining current sources (continued) Key point: Current sources should not be placed in series (unless they have the same current). Example: This is an improper connection. What law is violated here? 2A 6A Practical exception: Current sources of the same value could be placed in series to increase the total voltage capability. For example, suppose that two 10A current sources each have Vmax = 100V and they are placed in series. Illustrate.

  34. Chapter 2 EGR 271 – Circuit Theory I 34 Valid versus invalid circuits The text makes a point that all circuits must always satisfy KVL and KCL. A circuit that does not satisfy KVL or KCL is invalid and would be impossible to construct (or the circuit or equipment might be damaged). A few initial problems in the text ask is a circuit is valid. To test this, simply check KVL around various paths and KCL at various nodes to insure that no invalid equations occur. Example: Is the following circuit valid? Example: Is the following circuit valid?

  35. Chapter 2 EGR 271 – Circuit Theory I 35 _ + V3 3 6A I1 I2 4 4 12V 40V Example: Find I1, I2, and V3 in the circuit shown below.

  36. Chapter 2 EGR 271 – Circuit Theory I 36 2 2 I3 + + 3A 1 2A V1 V2 9V _ _ Example: Find V1, V2, and I3 in the circuit shown below.Also show that Pgenerated = Pabsorbed for the circuit below (true for any circuit).

  37. Chapter 2 EGR 271 – Circuit Theory I 37 Example: Find ig, ia, vg, and the total power developed in the circuit shown below.

  38. Chapter 2 EGR 271 – Circuit Theory I 38 Example: If ia = 4A and ib = 2A, find ig, vg, and the power dissipated by each resistor.

  39. Chapter 2 EGR 271 – Circuit Theory I 39 Dependent Sources Dependent sources are sources whose values depend on other circuit variables, such as a voltage or a current elsewhere in the circuit. There are 4 types of dependent sources: Voltage-controlled voltage source– a voltage source whose values depends on some other voltage in the circuit Current-controlled voltage source– a voltage source whose values depends on some other current in the circuit Voltage-controlled current source– a current source whose values depends on some other voltage in the circuit Current-controlled current source– a current source whose values depends on some other current in the circuit Examples of each type of dependent source:

  40. Chapter 2 EGR 271 – Circuit Theory I 40 • When are Dependent Sources Used? • Dependent sources are not sources that you might buy from an electronics store. • They are mathematical models that are needed because some circuit devices act like dependent sources at times. For example, dependent sources are commonly used to model transistors and operational amplifiers. • Examples: Models for two devices are shown below. - V- Vo V+ + Bipolar Junction Transistor (BJT) Operational Amplifier What type of dependent source is used in this model? _________________ What type of dependent source is used in this model? _________________

  41. Chapter 2 EGR 271 – Circuit Theory I 41 Example: Solve for I1 and I2 in the circuit shown below.

  42. Chapter 2 EGR 271 – Circuit Theory I 42 Example: Solve for I1 and V1 in the circuit shown below.

  43. Chapter 2 EGR 271 – Circuit Theory I 43 Example: Show that Pgenerated = Pabsorbed for the circuit below.

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