Upload
adrian-johnson
View
217
Download
2
Tags:
Embed Size (px)
Citation preview
Fall 2001 Circuits I 1
Chapter 1 - Basic Concepts
• 1.1 System of Units
• 1.2 Basic Quantities
• 1.3 Circuit Elements
Fall 2001 Circuits I 2
Reading Assignment:
Chapter 1, Pages 1-11
HomeworkEnd-of-Chapter Problems: P1.13, P1.18, P1.21
(PLUS WebCT Problems)
Fall 2001 Circuits I 3
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
“Today we live in a predominately electrical world.”
Fall 2001 Circuits I 4
System of Units
Unit of Measure Symbol Measuresmeter m distance
kilogram kg mass (weight)second s timeampere A electric current
degree Kelvin K temperaturecandela cd luminous intensity
The international system of units (SI) is composed of the following basic units of measure:
Fall 2001 Circuits I 5
Standard SI PrefixesStandard 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 Power Prefix Powerpico (p) 10-12 kilo (k) 10+3
nano (n) 10-9 mega (M) 10+6
micro () 10-6 giga (G) 10+9
milli (m) 10-3 tera (T) 10+12
1 103 106 109 1012
kilo(k)
mega(M)
giga(G)
tera(T)
10-12 10-9 10-6 10-3
pico(p)
nano(n)
micro( or u)
milli(m)
Fall 2001 Circuits I 6
TI-85 MODE Function
To Select Engineering Notation
Fall 2001 Circuits I 7
Example - Using Engineering Notation
If the local power company charges $0.12 per kWh (kilowatt-hour) of energy used, how much would it cost to illuminate a 100-Watt lamp for an entire year?
Solution:
12.105$Cost
kWhper12.0$kWh876Cost
kWh876W
day
hours24days365W100W
)kWhorhourskW(tPW
TimePowerEnergy
TI-85 Screen
(Wh)
(kWh)
Fall 2001 Circuits I 8
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 9
DefinitionsCharge 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 10
Current has magnitude and direction.
Electrical Conductor Segment
2A
Conventional Current Flow
- - --
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 second2A 12,500,000,000,000,000,000 electrons per second
Fall 2001 Circuits I 11
Typical Current Magnitudes106
Lightning Bolt104
Large Industrial Motor Current102
Typical Household Appliance Current100
Causes Ventricular Fibrillation in Humans10-2
10-4
10-6
IC Memory Cell Current10-8
10-10
10-12
Synaptic Current (Brain Cell)10-14
Cu
rren
t in
Am
per
es (
A)
Fall 2001 Circuits I 12
Direct Current (dc) Versus Alternating Current (ac)
DC signals are constant with respect to time:
t
Ix
2A
AC signals vary with respect to time:
t
i(t)
2A
-1A
periodic ac signal
t
i(t) = 2e-at
2A
nonperiodic ac signal
Fall 2001 Circuits I 13
Charge - Current Relationships
t
0t
t
0t
t
0t
t
0t
t
0t
t
0t
d)(i)0
t(q)t(q
d)(i)0
t(q)t(q
d)(i)(q
d)(i)(dq
dt)t(i)t(dqdt
)t(dq)t(iCurrent is proportional to the rate of change of charge.
Charge is increased or decreaseddepending on the area under thecurrent function.
Fall 2001 Circuits I 14
Example 1
Given: q(t) = 12t CFind: 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 15
Example 2
Given: The current entering an element is described by thefunction in the graph shown below.
t
(seconds)
i(t)
1 2 3
1
2
3
1tt1t01)t(i
Find: The amount of change in the charge of the elementover the interval 0 to 3 seconds.
Fall 2001 Circuits I 16
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.
t
i(t)
1 2 3
1
2
3
C5)5.05.4()01(3
122t1
0
3
1
10
ttdtdt1Q
C5A2s221s3A1AreaQ
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 17
Definition - VoltageAs 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.
+
-
BatteryLamp
i (current flow)
+
Vab
-
+
Vab
-
i
b
a
Fall 2001 Circuits I 18
BatteryLamp
i (current flow)
+
Vab
-
+
Vab
-
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.
Fab
Fab
b
a
Fall 2001 Circuits I 19
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.
coulombjoule1volt1
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 20
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.
+
BatteryLamp
i+
6 V
-
+
6 V
-
“0” volts (ground)
(6 V above ground)
Fall 2001 Circuits I 21
Power and EnergyEnergy 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)
BatteryLamp
i
+
Vab
-
+
Vab
-
Fall 2001 Circuits I 22
dtdwp
Battery Lamp
power flows from the source to the load
+
V
-
+
V
-
i i
p = -vi
Supplies Power
p = +vi
Absorbs Power
(Passive sign convention)
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).
Fall 2001 Circuits I 23
Mathematical Relationships
In electrical terms:
velocityforcepower In general:
ondsecjoule1va1ampvolt1watt1
wattsivp
Using previous definitions:
dqdw
dtdq
dtdw
v
,sodtdqiand
dtdwpbut
ipv
Fall 2001 Circuits I 24
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.
t
t
t
t
t
t
0
0
00
pdt)t(w)t(w
pdtdw
pdtdwdtdwp
Fall 2001 Circuits I 25
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.
Solution: C2000]t10x2[dt10x2dt)t(iQ 1.00
41.0
0
1.0
0
4 (a)
TJ1J10x1VC10x10w
)V10x5()C2000(VQw1211
8
(b) ( )dw
v tdq
WV
Q
W V Q
Note,
If V is constant,
Then,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 26
Example 4 - (a) Find the power absorbed by the element shown and (b) the total energy absorbed over a 10-second interval.
10
0
J400dt40w(b)
10A + 4v -
Solution: p = vi =4v x 10A = 40w(a)
Fall 2001 Circuits I 27
Example 5 - Find the power absorbed or supplied by the elements shown below
Solution: (a) p = -vi = -2v x 4A = -8w(element-a is supplying 8w of power)
4A - 2v +(a)
+ 2v -(b)
-2A
(b) p = -vi = -2v x (-2A) = +4w(element-b is absorbing 4w of power)
Fall 2001 Circuits I 28
Example 6 - Determine the unknown voltage or current.
Solution:(a) -20w = -V x 5A
V = 4v
5A - V=? +(a)
- 5v +(b)
I=?
P = -20w P = 40w
(b) 40w = -(5v x I)I = -8A
Fall 2001 Circuits I 29
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 30
Independent Voltage Sources:
+V-
Constant (battery)
LOAD
I
+v(t)
-
+-
Time-varying
LOAD
i(t)
p
v
V
Since p = vi, as the demand for power increases, the current, i, increases because v is constant.
Fall 2001 Circuits I 31
Independent Current Sources:
p
i
I
Since p = vi, as the demand for power increases, the voltage,v, increases because i is constant.
+v(t)orV-
LOADi(t)orI
Fall 2001 Circuits I 32
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 T is the temperature and k is a constant,
Fall 2001 Circuits I 33
Dependent SourcesThere are four types of controlled sources:
voltage-controlled voltage sources (VCVS)current-controlled voltage sources (CCVS)voltage-controlled current sources (VCCS)current-controlled current sources (CCCS)
+vo
-
+-
+v = vo
-
VCVS
io
+-
+v = rio
-
CCVS
Fall 2001 Circuits I 34
Dependent Sources
VCCS+vo
-
i = gvo
CCCSi =vo
io
Fall 2001 Circuits I 35
Example 7 - Given the two networks shown below we want to determine the outputs.
Solution:
(a) Vo = 20 2V = 40V
(b) Io = 50 1mA = 50mA
+Vs = 2V
-
+-
+Vo= 20Vs
-
(a)
(b)
50Is
Is = 1mA Io
Fall 2001 Circuits I 36
Example 8 - Compute the power that is supplied or absorbed by each element in the network below.
Solution:
P36V = -(36V)(4A) = -144W (supplies 144W)P1 = +(12V)(4A) = +48W (absorbs 48W)P2 = +(24V)(2A) = +48W (absorbs 48W)PDS = -(4V)(2A) = -8W (supplies 8W)P1 = +(28V)(2A) = +56W (absorbs 56W)Total = 0W
1Ix
+
-
1
2 3
- +
Ix = 4A2A
2A
+
24V
-
+
36V
-
+
28V
-
+ 12V -
Fall 2001 Circuits I 37
Example 9 - Determine the value of Io.
Solution:
P2A = -(6V)(2A) = -12W P1 = +(6V)(Io) = 6IoW = ? P2 = -(12V)(9A) = -108W P3 = -(10V)(3A) = -30WP4V = -(4V)(8A) = -32W PDS = +(16V)(11A) = 176WSince PTotal = 0W = -182 + 6Io + 176 6Io = 6W Io = 1A
- 6V +
+
-
1 2
3+
-8Ix
Ix = 2A
2A
+
10V
-
+
4V
-
+ 6V - - 12V +9AIo
8A3A
11A