Lecture Notes - PowerPoint PPT Presentation

About This Presentation
Title:

Lecture Notes

Description:

ECE 206L Lecture Notes * ECE 206L – PowerPoint PPT presentation

Number of Views:145
Avg rating:3.0/5.0
Slides: 76
Provided by: D4050
Category:

less

Transcript and Presenter's Notes

Title: Lecture Notes


1
ECE 206L
  • Lecture Notes



1
2
DC Current vs. AC Current 
  • Direct current (DC) flows in one direction the
    circuit. 
  • Alternating current (AC) flows first in one
    direction then in the opposite direction.
  • The same definitions apply to alternating voltage
    (AC voltage) 
  • DC voltage has a fixed polarity.
  • AC voltage switches polarity back and forth.
  • There are numerous sources of DC and AC current
    and voltage. However  Sources of DC are commonly
    shown as a cell or battery, and for the AC
    current Generators 

2
3
The Sinusoidal AC Waveform
  • The most common AC waveform is a sine (or
    sinusoidal) waveform.   
  • The vertical axis represents the amplitude of the
    AC current or voltage, in amperes or volts. 
  • The horizontal axis represents the angular
    displacement of the waveform. The units can be
    degrees or radians. 
  • The sine waveform is accurately represented by
    the sine function of plane trigonometry  y
    rsinq
  • where  y the instantaneous amplitude
  • r the maximum amplitude
  • q the horizontal
    displacement

3
4
DefinitionPeak and Peak-to-Peak Voltage 
  •     
  • Peak and peak-to-peak values are most often used
    when measuring the amplitude of ac waveforms
    directly from an oscilloscope display.
  • Peak voltage is the voltage measured from the
    baseline of an ac waveform to its maximum, or
    peak, level.  Unit Volts peak (Vp)  Symbol Vp
  • For a typical sinusoidal waveform, the positive
    peak voltage is equal to the negative peak
    voltage.   Peak voltages are expressed without a
    or - sign.
  •  
  • Peak-to-peak voltage is the voltage measured from
    the maximum positive level to the maximum
    negative level.  Unit Volts peak-to-peak 
    (Vp-p)  Symbol Vp-p
  • For a typical sinusoidal waveform, the
    peak-to-peak voltage is equal to 2 times the peak
    voltage.  Peak-to-peak voltages are expressed
    without a or - sign .

4
5
Conversion
  • Convert Vp to Vp-p  Vp-p 2 Vp
  • Convert Vp-p to Vp  Vp 0.5Vp-p
  • What is the peak-to-peak value of a sinusoidal
    waveform that has a peak value of 10 V? 
  • What is the peak value of a sine wave that has a
    peak-to-peak value of 240 V?   

5
6
Instantaneous Current and Voltage 
  • i Ipsin?
  • Where  
  • i instantaneous current in amperes  Ip
    the maximum, or peak, current in amperes  ?
    the angular displacement in degrees or radians
  • v Vpsin?
  • Where 
  • v instantaneous voltage in volts  Vp
    the maximum, or peak, voltage in volts  ? the
    angular displacement in degrees or radians

6
7
Average Voltage
  • Average voltage is the average value of all the
    values for one half-cycle of the waveform.  Unit
    Volts average (Vave)  Symbol Vave 
  • The average voltage of a sinusoidal waveform is
    equal to 0.637 times its peak value. 
  • Vave 0.637Vp
  • The average voltage is determined from just one
    half-cycle of the waveform because the average
    value of a full cycle is zero.  Average voltages
    are expressed without a or - sign 

7
8
Average Voltage
  • Convert Vp to Vave  Vave 0.637Vp 
  • Convert  Vave to Vp Vp 1.57Vave
  • Determine the average value of a waveform that
    measured 16 Vp.  Ans 10.2 Vave
  • What is the peak value of a waveform that has an
    average value of 22.4 V?  Ans 35.1 Vp

8
9
Root-Mean-Square (RMS) Voltage 
  •  
  • AC levels are assumed to be expressed as RMS
    values unless clearly specified otherwise.
  • RMS voltage is the amount of dc voltage that is
    required for producing the same amount of power
    as the ac waveform.  Unit Volts (V)  Symbol
    Vrms 
  • The RMS voltage of a sinusoidal waveform is equal
    to 0.707 times its peak value. 
  • Vrms 0.707Vp
  • In a dc circuit, applying 2 V to a 1 W resistance
    produces 4 W of power.   In an ac circuit,
    applying 2 Vrms to a 1 W  resistance produces 4 W
    of power. 
  • RMS voltages are expressed without a or -
    sign. 

9
10
ConversionRoot-Mean-Square (RMS) Voltage 
  • Convert Vp to Vrms  Vrms 0.707Vp 
  • Convert Vrms to Vp   Vp 1.414Vrms 
  • Determine the RMS value of a waveform that
    measures 15 Vp.  Ans 10.6 V
  • Determine the peak value of 120 V.
    .
  • (Assume 120 V is in RMS)  Ans 170 Vp

10
11
Resistors in Series
11
12
Resistors in Parallel
12
13
Measuring Voltage
Total Voltage VR1VR2
13
14
Voltage Dividers
The voltage is divided up in such that it is
proportional to the resistances of the resistors
in a series circuit.
14
15
Statistical Evaluation of Measurement Data and
Errors
  • Average or mean value of a set of measurement
  • Deviation from the average value
  • Average value of the deviation
  • Standard deviation(from the concept of RMS)
  • Probability of error size in one observation

16
The Decibel (dB)
  • The decibel, or dB, is a means of expressing
    the gain of an active device (such as an
    amplifier) or the loss in a passive device (such
    as an attenuator or length of cable). It is
    simply the ratio of output to input expressed in
    logarithmic form. The decibel was developed by
    the telephone company(Bel, to express the gain or
    loss in telephone transmission systems.

17
Calculating the Decibel (dB)
  • Now, imagine for a moment what it would be like
    to calculate the total gain of a string of
    amplifiers. It would be a cumbersome task at
    best, and especially so if there were portions of
    the cascade which were lossy and reduced the
    total gain, thereby requiring division as well as
    multiplication.
  • log (A x B) log A log B
  • log (A/B) log A - log B
  • Using the Decibel
  •                     
  • G 10 log (Po/Pi)     ,
  • Where
  • G Gain in dB
  • Po Power output from the device
  • Pi Power input to the device
  • Ex. A length of coaxial transmission line is
    being fed with 150 watts from a transmitter, but
    the power measured at the output end of the line
    is only 112 watts. What is the line loss in dB?
  • G 10 log (112/150)
  • G 10 log 0.747
  • G 10 (-0.127)
  • G -1.27 dB
  •                          

18
Capacitors
  • Capacitors consist of two plates with a
    dielectric material in-between. When a potential
    difference is placed across the plates, a charge
    builds up until it is large enough to cause a
    discharge across the plates through the material.

18
19
Reading Capacitors
Larger capacitors have the number of microfarads
written on them directly. Smaller capacitors use
a code based on the number of picofarads. We
generally use microfarads, so XYZ
XY 10Z 10-6 mF
19
20
Capacitors in Series
20
21
Capacitors in Parallel
21
22
Impedance vs. Resistance
  • Resistance is a property of a material that
    causes a reduction in the rate of flow of
    electrons.
  • Impedance is the reduction in the rate of flow of
    electrons caused by the material (resistance) AND
    other the properties of the component involved
    (reactance).
  • Resistors have no reactance. So the impedance of
    a resistor is equal to its resistance only.
  • Reactance varies with the frequency of the input.
    Resistance remains the same at all frequencies.
  • Both impedance and resistance are measured in
    ohms.

23
ImpedanceDefinition
  • A general measure of how a component or group of
    components pushes against the current flowing
    through it.
  • Impedance resistance reactance
  • Impedance is used to refer to the behavior of
    circuits with resistors, capacitors and other
    components.
  • When we consider components in a theoretical
    circuit diagram, the impedance of inductors and
    capacitors is their reactance only. Any
    resistance is modeled separately as a resistor.
    So theoretical capacitors and inductors have
    impedance, but no resistance.

24
Capacitor Impedance
Real capacitors have effectively no resistance,
so impedance is reactance for all capacitors.
24
25
What is Reactance
  • Reactance is the property of resisting or
    impeding the flow of ac current or ac voltage in
    inductors and capacitors. Note particularly we
    speak of alternating current only ac, which
    expression includes audio af and radio
    frequencies rf. NOT direct current dc.
  • Inductive Reactance
  • When ac current flows through an inductance a
    back emf or voltage develops opposing any change
    in the initial current. This opposition or
    impedance to a change in current flow is measured
    in terms of inductive reactance. 2 pi f L
  • where 2 pi 6.2832 f frequency in hertz
    and L inductance in Henries
  • Capacitive Reactance
  • When ac voltage flows through a capacitance an
    opposing change in the initial voltage occurs,
    this opposition or impedance to a change in
    voltage is measured in terms of capacitive
    reactance. 1 / (2 pi f C)
  • where 2 pi 6.2832 f frequency in hertz
    and C capacitance in Farads

26
Some examples of Reactance
  • What reactance does a 6.8 uH inductor present at
    7 Mhz? Using the formula above we get
  • 2 pi f L
  • where 2 pi 6.2832 f 7 X 106 Hz and L
    6.8 X -6 Henries
  • Answer 299 ohms
  • What reactance does a 33 pF capacitor present at
    7 Mhz? Using the formula above we get
  • 1 / (2 pi f C)
  • where 2 pi 6.2832 f 7 X 106 Hz and C
    33 X -12 Farads
  • Answer 689 ohms

27
Inductors
An inductor is a coil of wire through which a
current is passed. The current can be either AC
or DC.
27
28
Inductors
This generates a magnetic field, which induces a
voltage proportional to the rate of change of the
current.
28
29
Combining Inductors
  • Inductances add like resistances
  • Series
  • Parallel

29
30
Inductor Impedance
Real inductors always have a small resistance
(that is not shown in these circuits). The
impedance of the theoretical inductor shown is
only its reactance.
30
31
Comparison of Components
32
ImpedanceDefinition
  • A general measure of how a component or group of
    components pushes against the current flowing
    through it.
  • Impedance resistance reactance
  • Impedance is used to refer to the behavior of
    circuits with resistors, capacitors and other
    components.
  • When we consider components in a theoretical
    circuit diagram, the impedance of inductors and
    capacitors is their reactance only. Any
    resistance is modeled separately as a resistor.
    So theoretical capacitors and inductors have
    impedance, but no resistance.

33
Equipment Impedances
  • Each measuring device changes the circuit when
    you use it.
  • The impedance of the device helps you understand
    how much.
  • Device Impedances
  • Function Generator 50 ohms
  • Scope 1Meg ohms
  • DMM (DC voltage) 10Meg ohms
  • DMM (AC voltage) 1Meg ohms
  • DMM (DC current) 5 ohms (negligible)

33
34
Effect of Impedance on Circuit
Function generator thinks it is putting out the
same thing.
Output is clearly different.
34
35
Effect of Impedance on Circuit
The function generator has an output impedance of
much less than 50O, so we can ignore it.
35
36
Kirchoffs Laws
sum of currents entering a junction is the same
as the sum of the currents leaving a junction
sum of voltages in any loop is zero
37
Circuit Analysis (Combination Method)
38
SI Suffixes
pico p 10-12
nano n 10-9
micro ? (u) 10-6
milli m 10-3
Kilo k 103
Mega M (Meg) 106
Giga G 109
Tera T 1012
39
Oscilloscope Tutorial
  • The oscilloscope is basically a graph-displaying
    device
  • It draws a graph of an electrical signal.
  • In most applications the graph shows how signals
    change over time
  • the vertical (Y) axis represents voltage
  • the horizontal (X) axis represents time.

40
Oscilloscopes
Horizontal sweeps at a constant rate. Vertical
plates are attached to an external voltage, the
signal you attach to the scope.
41
Cathode Ray Tubes
Variation in potential difference (voltage)
placed on plates causes electron beam to bend
different amounts. Sweep refers to refreshing
repeatedly at a fixed rate.
42
(No Transcript)
43
Scope (Cont)
  • This simple graph can tell you many things about
    a signal
  • You can determine the time and voltage values of
    a signal.
  • You can calculate the frequency of an oscillating
    signal.
  • You can see the "moving parts" of a circuit
    represented by the signal.
  • You can tell if a malfunctioning component is
    distorting the signal.
  • You can find out how much of a signal is direct
    current (DC) or alternating current (AC).
  • You can tell how much of the signal is noise and
    whether the noise is changing with time.

44
(No Transcript)
45
How does an Analog Scope work?
46
How does a Digital Scope work?
47
Triggering Stabilizes a Repeating Waveform
48
Waveform shapes tell you a great deal about a
signal
49
If a signal repeats, it has a frequency. The
frequency is measured in Hertz (Hz) and equals
the number of times the signal repeats itself in
one second
50
Voltage, Current, Phase
51
Performance Terms
  • Bandwidth
  • The bandwidth specification tells you the
    frequency range the oscilloscope accurately
    measures.
  • Rise Time
  • Rise time may be a more appropriate performance
    consideration when you expect to measure pulses
    and steps. An oscilloscope cannot accurately
    display pulses with rise times faster than the
    specified rise time of the oscilloscope.
  • Vertical Sensitivity
  • The vertical sensitivity indicates how much the
    vertical amplifier can amplify a weak signal.
    Vertical sensitivity is usually given in
    millivolts (mV) per division.
  • Sweep Speed
  • For analog oscilloscopes, this specification
    indicates how fast the trace can sweep across the
    screen, allowing you to see fine details. The
    fastest sweep speed of an oscilloscope is usually
    given in nanoseconds/div.
  • Gain Accuracy
  • The gain accuracy indicates how accurately the
    vertical system attenuates or amplifies a signal.
  • Time Base or Horizontal Accuracy
  • The time base or horizontal accuracy indicates
    how accurately the horizontal system displays the
    timing of a signal.
  • Sample Rate
  • On digital oscilloscopes, the sampling rate
    indicates how many samples per second the ADC can
    acquire. Maximum sample rates are usually given
    in megasamples per second (MS/s). The faster the
    oscilloscope can sample, the more accurately it
    can represent fine details in a fast signal..
  • ADC Resolution (Or Vertical Resolution)
  • The resolution, in bits, of the ADC indicates how
    precisely it can turn input voltages into digital
    values.
  • Record Length
  • The record length of a digital oscilloscope
    indicates how many waveform points the
    oscilloscope is able to acquire for one waveform
    record.

52
Grounding
  • Proper grounding is an important step when
    setting up to take measurements.
  • Properly grounding the oscilloscope protects you
    from a hazardous shock and protects your circuits
    from damage.
  • Grounding the oscilloscope is necessary for
    safety. If a high voltage contacts the case of an
    ungrounded oscilloscope, any part of the case,
    including knobs that appear insulated, it can
    give you a shock. However, with a properly
    grounded oscilloscope, the current travels
    through the grounding path to earth ground rather
    than through you to earth ground.
  • To ground the oscilloscope means to connect it to
    an electrically neutral reference point (such as
    earth ground). Ground your oscilloscope by
    plugging its three-pronged power cord into an
    outlet grounded to earth ground.
  • Grounding is also necessary for taking accurate
    measurements with your oscilloscope. The
    oscilloscope needs to share the same ground as
    any circuits you are testing.
  • Some oscilloscopes do not require the separate
    connection to earth ground. These oscilloscopes
    have insulated cases and controls, which keeps
    any possible shock hazard away from the user.

53
Scope Probes Most passive probes have some
degree of attenuation factor, such as 10X, 100X,
and so on. By convention, attenuation factors,
such as for the 10X attenuator probe, have the X
after the factor. In contrast, magnification
factors like X10 have the X first
54
Vertical Controls
  • Position and Volts per Division
  • The vertical position control lets you move the
    waveform up or down to exactly where you want it
    on the screen.
  • The volts per division (usually written
    volts/div) setting varies the size of the
    waveform on the screen. A good general purpose
    oscilloscope can accurately display signal levels
    from about 4 millivolts to 40 volts.
  • Often the volts/div scale has either a variable
    gain or a fine gain control for scaling a
    displayed signal to a certain number of
    divisions.

55
Input Coupling
  • Coupling means the method used to connect an
    electrical signal from one circuit to another.

56
Horizontal Controls
  • Position and Seconds per Division
  • The horizontal position control moves the
    waveform from left and right to exactly where you
    want it on the screen.
  • The seconds per division (usually written as
    sec/div) setting lets you select the rate at
    which the waveform is drawn across the screen
    (also known as the time base setting or sweep
    speed). This setting is a scale factor. For
    example, if the setting is 1 ms, each horizontal
    division represents 1 ms and the total screen
    width represents 10 ms (ten divisions). Changing
    the sec/div setting lets you look at longer or
    shorter time intervals of the input signal.

57
Trigger Position
  • The trigger position control may be located in
    the horizontal control section of your
    oscilloscope. It actually represents "the
    horizontal position of the trigger in the
    waveform record." Horizontal trigger position
    control is only available on digital
    oscilloscopes.
  • Varying the horizontal trigger position allows
    you to capture what a signal did before a trigger
    event (called pretrigger viewing).
  • Digital oscilloscopes can provide pretrigger
    viewing because they constantly process the input
    signal whether a trigger has been received or
    not. A steady stream of data flows through the
    oscilloscope the trigger merely tells the
    oscilloscope to save the present data in memory.
    I
  • n contrast, analog oscilloscopes only display the
    signal after receiving the trigger.

58
Trigger Controls (cont)
59
Pulse and Rise Time Measurements
60
Multimeter tutorial
  • A meter is a measuring instrument. An ammeter
    measures current, a voltmeter measures the
    potential difference (voltage) between two
    points, and an ohmmeter measures resistance.
  • A multimeter combines these functions, and
    possibly some additional ones as well, into a
    single instrument.

61
To measure current, the circuit must be broken to
allow theammeter to be connected in
series Ammeters must have a LOW resistance
62
To measure potential difference (voltage), the
circuit is not changed the voltmeter is
connected in parallelVoltmeters must have a
HIGH resistance
63
To measure resistance, the component must be
removed from the circuit altogether Ohmmeters
work by passing a current through the component
being tested
64
Digital MultimetersDigital meters give an
output in numbers, usually on a liquid crystal
display.Most modern multimeters are digital and
traditional analogue types are destined to become
obsolete.Digital multimeters come in a wide
range of sizes and capability. Everything from
simple 3 ½ digit auto ranging pocket meters to
larger 8 ½ digit bench model with operator or
computer (IEEE488 compatible) settable range
selection
65
(No Transcript)
66
Function Generator
  • An electronic instrument that generates various
    waveforms such as
  • Sine wave
  • Square wave
  • Pulse trains
  • Sawtooth
  • The amplitude, DC offset, frequency are
    adjustable.

67
Function Generators (cont)
  • Like multimeters there is a wide variety of
    device offering various
  • Amplitude characteristics
  • Bandwidth
  • Adjustments of rise and fall times
  • Modulation capability (AM, FM, Pulse, etc.)

68
Power Supply
  • This is the device that transfers electric power
    from a source to a load using electronic
    circuits.
  • Typical application of power supplies is to
    convert utility's AC input power to a regulated
    voltage(s) required for electronic equipment.
  • Depending on the mode of operation of power
    semiconductors PS can be linear or switching.
  • In a switched-mode power supply, or SMPS power
    handling electronic components are continuously
    switching on and off with high frequency in order
    to provide the transfer of electric energy. By
    varying duty cycle, frequency or a phase of these
    transitions an output parameter (such as output
    voltage) is controlled. Typical frequency range
    of SMPS is from 20 kHz to several MHz.

69
Power Supply (cont)
  • Power supplies like many of the other electronic
    instruments, come in many varieties with a wide
    range of capabilities
  • Parameters that are Power Supply specific
    include
  • Voltage levels
  • Current
  • Regulation
  • Protection
  • Output impedance
  • Noise (ripple)
  • Its the designer (or researcher) responsibility
    to identify the characteristics required.

70
Oscilloscope
71
Oscilloscope(continue)
  • ?DEMO.Lab3a

72
Capacitance (continue from before)
  • A capacitor simply consists of two conductors
    which are electrically isolated from one
    another.  This means that no current can readily
    flow from one conductor to the other.
  • the units of the capacitance must equal one
    coulomb per volt, which is defined to be one
    farad, F
  • One Farad one(coulomb/volts)
  • 1F1C/V

73
RC Circuitsqualitative description
assume the switch is thrown to position B at the
time t   0.  When the switch is at the position
B the circuit consists of the single loop which
contains, starting at point B and moving around
the circuit clockwise, the resistor R, the
capacitor C, and  finally the voltage source
DVs.  In this configuration the voltage source
attempts to push charge  around the circuit in a
clockwise direction (remember that the power
source tries to push current out of its positive
terminal).
74
RC Circuitsqualitative description(continue)
After some time at position B, we will throw the
switch to position A.  (The time since the switch
was thrown to position A is called a new time t
.  The prime on a symbol is used to denote
the fact that this is the value of the quantity
under consideration since the switch was thrown
to position A.  It therefore follows that the
switch is thrown to the position A at the time t
0.) After the switch has been thrown to
position A the circuit consists solely of the
resistor and the capacitor, with no voltage
source. In this case there is no external energy
being used to move charges around the circuit
loop.
75
RC Circuitsqualitative description(continue)
The behavior of the voltage across the capacitor
as a function of time and the current around the
circuit (and in particular, through the resistor)
as a function of time for the case in which the
switch has been thrown to position B.  (This is
the case of the charging capacitor.) Then after
that is the case in which the switch has been
thrown to position A (the case of the discharging
capacitor).
Write a Comment
User Comments (0)
About PowerShow.com