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Chapter 1 - Basic Concepts • 1.1 System of Units • 1.2 Basic Quantities • 1.3 Circuit Elements Fall 2001 Circuits I 1 Reading Assignment: Chapter 1, Pages 1-11 Homework End-of-Chapter Problems: P1.13, P1.18, P1.21 (PLUS WebCT Problems) Fall 2001 Circuits I 2 “Today we live in a predominately electrical world.” Electrotechnology pervades our day-to-day lives: electrical appliances Refrigerators, stoves, stereos, hairdryers, ... communication devices telephones, faxes, computer and data networks computers main frames, personal (PCs), workstations, embedded systems, PLCs instrumentation meters, measurement systems, controls Fall 2001 Circuits I 3 System of Units The international system of units (SI) is composed of the following basic units of measure: Unit of Measure meter kilogram second ampere degree Kelvin candela Fall 2001 Symbol m kg s A K cd Circuits I Measures distance mass (weight) time electric current temperature luminous intensity 4 Standard SI Prefixes Standard prefixes are employed with SI units to represent powers of ten. These prefixes, sometimes referred to as engineering notation, are used extensively in representing the values of various circuit parameters. Prefix pico (p) nano (n) micro () milli (m) Power 10-12 10-9 10-6 10-3 10-12 10-9 10-6 10-3 pico nano micro milli (p) (n) ( or u) (m) Fall 2001 Prefix kilo (k) mega (M) giga (G) tera (T) 1 103 106 Power 10+3 10+6 10+9 10+12 109 1012 kilo mega giga tera (k) (M) (G) (T) Circuits I 5 TI-85 MODE Function To Select Engineering Notation Fall 2001 Circuits I 6 Example - Using Engineering Notation If the local power company charges $0.12 per kWh (kilowatt-hour) of energy used, how much would it cost to illuminate a 100-Watt lamp for an entire year? Solution: Energy Power Time W P t (kW hours or kWh ) 24hours W 100W 365days day W 876kWh Cost 876kWh $0.12 per kWh Cost $105.12 Fall 2001 TI-85 Screen (Wh) (kWh) Circuits I 7 Basic Quantities • What is Electricity? - A natural force (like wind or water flow) which can be harnessed for some beneficial purpose. • What causes electricity? Just as wind is due to the movement of air molecules, electricity is caused by the movement of charged particles (i.e., electrons). • The study of electricity has been going on since about 600 B.C. when it was noticed that amber, when rubbed, acquired the ability to pick up light objects (we call this static electricity). Fall 2001 Circuits I 8 Definitions Charge is an intrinsic property of matter (like mass and size). Symbol1: q or Q Unit: coulomb (C) The elemental unit of charge is the charge of one electron, e: e = -1.6022 x 10-19 C (1 proton = +1.6022 x 10-19 C) Current is a measure of the amount of charge flowing past a point in a given amount of time. Symbol1: i or I Unit: ampere (A) 1A 1C/s (coulomb per second) 1Lowercase is used to indicate a variable (time-dependent) quantity while upper case indicates a constant value. Fall 2001 Circuits I 9 Current has magnitude and direction. - - 2A Conventional Current Flow - - Electrical Conductor Segment Electron Flow (The flow of electrons is analogous to the flow of water molecules in a pipe or hose.) Note: 2A = 2C per second = (2/1.6022E-19) electrons per second 2A 12,500,000,000,000,000,000 electrons per second Fall 2001 Circuits I 10 Typical Current Magnitudes 106 Lightning Bolt 4 10 Large Industrial Motor Current 2 Current in Amperes (A) 10 Typical Household Appliance Current 0 10 Causes Ventricular Fibrillation in Humans -2 10 10-4 10-6 IC Memory Cell Current -8 10 10-10 10-12 Synaptic Current (Brain Cell) 10 Fall 2001 -14 Circuits I 11 Direct Current (dc) Versus Alternating Current (ac) DC signals are constant with respect to time: Ix 2A t AC signals vary with respect to time: i(t) = 2e-at i(t) 2A 2A -1A t t periodic ac signal Fall 2001 nonperiodic ac signal Circuits I 12 Charge - Current Relationships Current is proportional to the rate of change of charge. i(t) dq(t) dt dq(t) i(t)dt t t 0 0 t dq() t i()d t t t q() i()d t 0 0 t q(t) q(t ) i()d 0 t0 t q(t) q(t ) i()d 0 t0 Fall 2001 Charge is increased or decreased depending on the area under the current function. Circuits I 13 Example 1 Given: Find: q(t) = 12t C i(t) Solution: Since current is proportional to the rate of change of charge, we take the derivative of q(t) to find i(t): i(t) = q(t) i(t) = 12 A Since the slope (rate of change) of q(t) is constant at 12 Coulombs per second, the current is constant. Fall 2001 Circuits I 14 Example 2 Given: The current entering an element is described by the function in the graph shown below. i(t) 3 i(t) 1 0 t 1 t t 1 2 1 1 2 3 t (seconds) Find: The amount of change in the charge of the element over the interval 0 to 3 seconds. Fall 2001 Circuits I 15 Example 2 - Solution To find the change in the charge of the element, we need to find the area under the function i(t) over the interval 0 to 3 s. This can be done two ways for this example: by integration or by using area formulas for rectangles and triangles. i(t) Q Area 1A 3s 1 2s 2A 5C 2 3 2 1 3 Q 1dt tdt t 1 t (1 0) (4.5 0.5) 5C 0 2 1 0 1 3 2 1 1 2 3 t Note: 5C is the increase in the charge of the element. We must know the initial charge to determine the total charge of the element. Fall 2001 Circuits I 16 Definition - Voltage As stated earlier, current is the flow of charge through a conductor. Voltage is the force required to move the charge through the conductor. Hence, voltage is also referred to as electromotive force and potential difference. i (current flow) + a + Vab Battery + Lamp b - Vab - i Fall 2001 Circuits I 17 i (current flow) + + Vab Battery Vab Lamp - - The current from the battery flows through a voltage rise since the battery is supplying energy. There is an equal voltage drop across the lamp since the lamp is absorbing the energy supplied by the battery. This is similar to the counter force created by friction when pushing an object up an incline. a Fab Fab b Fall 2001 Circuits I 18 Electromotive force is measured in volts. If one joule of energy is required to move one coulomb of charge through an element, then there is one volt (V) of potential difference across the element. 1volt 1 joule coulomb Like current, the voltage across an element may be positive or negative. The assignment of a sign to a voltage is somewhat arbitrary, but usually represents whether potential difference is above or below some reference potential. Fall 2001 Circuits I 19 (6 V above ground) i + + + 6V Battery Lamp 6V - - “0” volts (ground) As we traverse the circuit in a clockwise direction, there is a voltage rise across the battery; we could assign this a “positive” sign. Since we experience a voltage drop across the lamp, this would be assigned the opposite sign or a “negative” value. We could just as correctly assign all voltage drops a positive sign and, therefore, all voltage rises a negative sign. Fall 2001 Circuits I 20 Power and Energy Energy is the capacity to do work. For example, energy is stored in a battery and, when connected to a “load” such as a lamp, there is a continuous exchange of energy from the battery to the load. (There is also a transformation from energy stored in a chemical form to energy emitted in the form of heat and light.) Typically, electrical energy is measure in joules (J) or watt-hours (W-h). (1W = 1J/s) i + Vab + Battery Lamp - Fall 2001 Vab Circuits I 21 Power is a measure of how much work is done per unit time, or, in other words, a measure of the rate at which energy is transferred (supplied or absorbed). There is always a conservation of energy (power). That is, the battery supplies exactly the amount of power consumed by the load, no more no less. Typically, electrical power is measured in watts (W). power flows from the source to the load p dw dt + V i + i Battery - (Passive sign convention) Fall 2001 Lamp V - p = -vi p = +vi Supplies Power Absorbs Power Circuits I 22 Mathematical Relationships In general: power force velocity In electrical terms: p v i watts 1watt 1volt amp 1va 1 joule sec ond Using previous definitions: Fall 2001 v p i but p dw and i dq dt dt so, dw dt dw v dq dq dt Circuits I 23 p dw dt dw pdt t t t0 t0 dw pdt t w(t) w(t ) pdt 0 t0 The total energy absorbed or supplied is equal to the area under the power function in the interval t0 to t. If the area is positive, then energy is absorbed by an element; if the area is negative, the element is supplying power. Fall 2001 Circuits I 24 Example 3 - The current in a typical lightening bolt is 20KA, and the bolt lasts typically for 0.1 seconds. If the voltage between the earth and clouds is 500MV, find (a) the total charge transmitted by the bolt and (b) the total energy released by the bolt. 4 4 Solution: (a) Q i(t)dt 2x10 dt [2x10 t]00.1 2000C 0.1 0.1 0 0 8 w Q V ( 2000 C ) ( 5 x 10 V) (b) 11 Note, v (t ) 12 w 10x10 C V 1x10 J 1TJ dq If V is constant, A typical automobile battery is rated at 12V and 100 amp-hours (Ah). 100Ah = (100 C/s)(3600s) = 3.6 105C 12V3.6 105C = 4.32 106J (MJ) The lightening strike has as much energy as 230,000 batteries! Fall 2001 Circuits I dw Then, V W Q W V Q 25 Example 4 - (a) Find the power absorbed by the element shown and (b) the total energy absorbed over a 10-second interval. 10A + Solution: (a) 4v - p = vi =4v x 10A = 40w (b) w 40dt 400J 10 0 Fall 2001 Circuits I 26 Example 5 - Find the power absorbed or supplied by the elements shown below 4A - 2v + -2A + 2v - (a) Solution: (b) (a) p = -vi = -2v x 4A = -8w (element-a is supplying 8w of power) (b) p = -vi = -2v x (-2A) = +4w (element-b is absorbing 4w of power) Fall 2001 Circuits I 27 Example 6 - Determine the unknown voltage or current. 5A - V=? + I=? (a) (b) P = -20w Solution: Fall 2001 - 5v + P = 40w (a) -20w = -V x 5A V = 4v (b) 40w = -(5v x I) I = -8A Circuits I 28 Circuit Elements • Circuits (electrical systems) consist interconnected devices. • Electrical devices can be categorized as either a source or a load. • A source can be either independent or dependent, a voltage source or a current source. • Independent voltage sources provide power at a constant voltage • Independent current sources provide power at a constant current. • The voltage level of a voltage source is not affected by the amount of power demanded from it. • Similarly, the current level of a current source is not affected by the amount of power demanded from it. Fall 2001 Circuits I 29 Independent Voltage Sources: I i(t) + v(t) - + - LOAD Time-varying + V - LOAD Constant (battery) v Since p = vi, as the demand for power increases, the current, i, increases because v is constant. Fall 2001 V p Circuits I 30 Independent Current Sources: + v(t) or V - i(t) or I LOAD i Since p = vi, as the demand for power increases, the voltage,v, increases because i is constant. Fall 2001 I p Circuits I 31 Dependent Source (Controlled) Sources) An independent source provides power to a circuit at a constant voltage or current, and the level of that voltage or current is unaffected by the circuit to which it is attached. Generally, independent sources are used to represent devices such as batteries or generators. A voltage or current associated with a dependent source is controlled or affected by the circuit to which it is attached. Dependent sources, also called controlled sources, are used to model electronic devices, sensors and other devices which are influenced by some physical or electrical parameter. For example, a device called a thermocouple generates a small voltage (in the millivolt range) which is proportional to temperature. So, a thermocouple can be thought of as a temperature-controlled voltage source. That is, v(t) = KT, where TFall is 2001 the temperature and k is aCircuits constant, I 32 Dependent Sources There are four types of controlled sources: voltage-controlled voltage sources current-controlled voltage sources voltage-controlled current sources current-controlled current sources VCVS + vo - + - CCVS io Fall 2001 + Circuits I (VCVS) (CCVS) (VCCS) (CCCS) + v = vo - + v = rio 33 Dependent Sources i = gvo VCCS + vo - i =vo CCCS io Fall 2001 Circuits I 34 Example 7 - Given the two networks shown below we want to determine the outputs. (a) + Vs = 2V - (b) Is = 1mA + - Solution: + Vo= 20Vs - (a) Vo = 20 2V = 40V Io (b) Io = 50 1mA = 50mA 50Is Fall 2001 Circuits I 35 Example 8 - Compute the power that is supplied or absorbed by each element in the network below. Ix = 4A 1Ix + 12V - 2A 1 + 36V - Solution: Fall 2001 - + + + 24V + 3 2 - - 2A P36V = -(36V)(4A) = -144W P1 = +(12V)(4A) = +48W P2 = +(24V)(2A) = +48W PDS = -(4V)(2A) = -8W P1 = +(28V)(2A) = +56W Total = 0W Circuits I 28V - (supplies 144W) (absorbs 48W) (absorbs 48W) (supplies 8W) (absorbs 56W) 36 Example 9 - Determine the value of Io. Ix = 2A - 6V + + 6V - 2A - 12V + Io 1 2 11A + + 10V 3A 9A 3 - 8A + 4V + - 8Ix - Solution: P2A = -(6V)(2A) = -12W P1 = +(6V)(Io) = 6IoW = ? P2 = -(12V)(9A) = -108W P3 = -(10V)(3A) = -30W P4V = -(4V)(8A) = -32W PDS = +(16V)(11A) = 176W Since PTotal = 0W = -182 + 6Io + 176 6Io = 6W Io = 1A Fall 2001 Circuits I 37