Lecture #1 OUTLINE Course overview Circuit Analysis.

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Presentation transcript:

Lecture #1 OUTLINE Course overview Circuit Analysis

Course Overview 1. Electrical quantities (review) Course content: Electric circuits 1. Electrical quantities (review) 2. Ideal basic circuit elements: Voltage and current sources Electrical resistance (Ohm’s law) 3. Power calculations 4. Kirchhoff’s Laws

Introduction to circuit analysis OUTLINE Electrical quantities Charge Current Voltage Power The ideal basic circuit element Sign conventions

Circuit Analysis Circuit analysis is used to predict the behavior of the electric circuit, and plays a key role in the design process. Design process has analysis as fundamental 1st step Comparison between desired behavior (specifications) and predicted behavior (from circuit analysis) leads to refinements in design In order to analyze an electric circuit, we need to know the behavior of each circuit element (in terms of its voltage and current) AND the constraints imposed by interconnecting the various elements.

Electric Charge Macroscopically, most matter is electrically neutral most of the time. Exceptions: clouds in a thunderstorm, people on carpets in dry weather, plates of a charged capacitor, etc. Microscopically, matter is full of electric charges. Electric charge exists in discrete quantities, integral multiples of the electronic charge 1.6 x 10-19 coulombs Electrical effects are due to separation of charge  electric force (voltage) charges in motion  electric flow (current)

Classification of Materials Solids in which all electrons are tightly bound to atoms are insulators. Solids in which the outermost atomic electrons are free to move around are metals. Metals typically have ~1 “free electron” per atom (~5 ×1022 free electrons per cubic cm) Electrons in semiconductors are not tightly bound and can be easily “promoted” to a free state. insulators semiconductors metals Quartz, SiO2 Si, GaAs Al, Cu dielectric materials excellent conductors

Electric Current Definition: rate of positive charge flow Symbol: i Units: Coulombs per second ≡ Amperes (A) i = dq/dt where q = charge (in Coulombs), t = time (in seconds)

Wire attached to end Example 1: Suppose we force a current of 1 A to flow from C1 to C2: Electrons flow is in -x direction: Wire attached to end

Electric Current Examples 105 positively charged particles (each with charge 1.6×10-19 C) flow to the right (+x direction) every nanosecond 105 electrons flow to the right (+x direction) every microsecond

Current Density Definition: rate of positive charge flow per unit area Symbol: J Units: A / cm2

Current Density Example Typical dimensions of integrated circuit components are in the range of 1 mm. What is the current density in a wire with 1 m² area carrying 5 mA?

Electric Potential (Voltage) Definition: energy per unit charge Symbol: v Units: Joules/Coulomb ≡ Volts (V) v = dw/dq where w = energy (in Joules), q = charge (in Coulombs) a Subscript convention: vab means the potential at a minus the potential at b. vab ≡ va - vb b

p = dw/dt = (dw/dq)(dq/dt) = vi Electric Power Definition: transfer of energy per unit time Symbol: p Units: Joules per second ≡ Watts (W) p = dw/dt = (dw/dq)(dq/dt) = vi Concept: As a positive charge q moves through a drop in voltage v, it loses energy energy change = qv

The Ideal Basic Circuit Element Polarity reference for voltage can be indicated by plus and minus signs Reference direction for the current is indicated by an arrow + v _ Attributes: Two terminals (points of connection) Mathematically described in terms of current and/or voltage Cannot be subdivided into other elements

Sign Convention for Power p = vi p = -vi i i i i _ v + _ v + + v _ + v _ If p > 0, power is being delivered to the box. If p < 0, power is being extracted from the box.

Power If an element is absorbing power (i.e. if p > 0), positive charge is flowing from higher potential to lower potential. i i _ v + + v _ or How can a circuit element absorb power? By converting electrical energy into heat (resistors in toasters), light (light bulbs), or acoustic energy (speakers); by storing energy (charging a battery).

Power Calculation Example Find the power absorbed by each element:

Summary Current = rate of charge flow Voltage = energy per unit charge created by charge separation Power = energy per unit time Ideal Basic Circuit Element 2-terminal component that cannot be sub-divided described mathematically in terms of its terminal voltage and current Sign convention Reference direction for current through the element is in the direction of the reference voltage drop across the element

Circuit Elements 5 ideal basic circuit elements: voltage source current source resistor inductor capacitor Many practical systems can be modeled with just sources and resistors The basic analytical techniques for solving circuits with inductors and capacitors are the same as those for resistive circuits active elements, capable of generating electric energy passive elements, incapable of generating electric energy

Electrical Sources An electrical source is a device that is capable of converting non-electric energy to electric energy and vice versa. Examples: battery: chemical electric dynamo (generator/motor): mechanical electric Electrical sources can either deliver or absorb power

Ideal Voltage Source Circuit element that maintains a prescribed voltage across its terminals, regardless of the current flowing in those terminals. Voltage is known, but current is determined by the circuit to which the source is connected. The voltage can be either independent or dependent on a voltage or current elsewhere in the circuit, and can be constant or time-varying. Circuit symbols: vs + vs=m vx + vs=r ix + _ _ _ independent voltage-controlled current-controlled

Ideal Current Source Circuit element that maintains a prescribed current through its terminals, regardless of the voltage across those terminals. Current is known, but voltage is determined by the circuit to which the source is connected. The current can be either independent or dependent on a voltage or current elsewhere in the circuit, and can be constant or time-varying. Circuit symbols: is is=a vx is=b ix independent voltage-controlled current-controlled

Electrical Resistance Resistance: Electric field is proportional to current density, within a resistive material. Thus, voltage is proportional to current. The circuit element used to model this behavior is the resistor. Circuit symbol: Units: Volts per Ampere ≡ ohms (W) The current flowing in the resistor is proportional to the voltage across the resistor: v = i R where v = voltage (V), i = current (A), and R = resistance (W) R (Ohm’s Law)

Electrical Conductance Conductance is the reciprocal of resistance. Symbol: G Units: siemens (S) or mhos ( ) Example: Consider an 8 W resistor. What is its conductance? W

Short Circuit and Open Circuit Wire (“short circuit”): R = 0  no voltage difference exists (all points on the wire are at the same potential) Current can flow, as determined by the circuit Air (“open circuit”): R =   no current flows Voltage difference can exist, as determined by the circuit

Circuit Nodes and Loops A node is a point where two or more circuit elements are connected. A loop is formed by tracing a closed path in a circuit through selected basic circuit elements without passing through any intermediate node more than once

Example: Power Absorbed by a Resistor p = vi = ( iR )i = i2R p = vi = v ( v/R ) = v2/R Note that p > 0 always, for a resistor. Example: Calculate the voltage vg and current ia. Determine the power dissipated in the 80W resistor.

More Examples Are these

Summary Current = rate of charge flow Voltage = energy per unit charge created by charge separation Power = energy per unit time Ideal Basic Circuit Elements 2-terminal component that cannot be sub-divided described mathematically in terms of its terminal voltage and current An ideal voltage source maintains a prescribed voltage regardless of the current in the device. An ideal current source maintains a prescribed current regardless of the voltage across the device. A resistor constrains its voltage and current to be proportional to each other: v = iR (Ohm’s law)