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Transcript
MALVINO & BATES
Electronic
PRINCIPLES
SEVENTH EDITION
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter
Introduction
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1
Topics Covered in Chapter 1
•
•
•
•
•
•
•
Three kinds of formulas
Approximations
Voltage sources
Current sources
Thevenin’s Theorem
Norton’s Theorem
Troubleshooting
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Three kinds of formulas
The definition:
Invented for a new concept
Q
C=
V
{defines what capacitance is}
{does not require verification}
The law:
Summarizes a relationship that exists in nature
f=K
The derivation:
Q1Q2
d2
{verified by experiment}
Obtained by manipulating other
formulas using mathematics
Q = CV
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Ideal voltage source
Maintains a constant output voltage, regardless of
the value of RL.
10 V
RL
VRL= 10 Volts
The ideal model can be called
the first approximation.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Approximations
• Widely used in industry
• Useful for troubleshooting
• Useful for circuit calculations
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Voltage Sources
• An ideal source has no internal resistance
• The second approximation of a voltage source
has internal resistance
• A stiff voltage source has an internal resistance
that is 1/100 of load resistance
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Real Voltage Source
Has an internal resistance in series with the source
RS
10 V
RL
VRL< 10 Volts
This model is called the
the second approximation.
When RL is equal to or greater than 100 times RS, a real
voltage source is stiff and the first approximation can be used.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Ideal current source
Maintains a constant
output current, regardless of the value of RL.
1A
RL
IRL= 1 Ampere
The ideal model can be called
the first approximation.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Real current source
Has a large internal resistance
in parallel with the source
1A
RS
RL
IRL< 1 Ampere
This model is called the
the second approximation.
When RS is equal to or greater than 100 times RL, a real
current source is stiff and the first approximation can be used.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Thevenin’s Theorem
• Used to replace any linear circuit with an
equivalent voltage source called VTH and an
equivalent resistance called RTH
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Thevenin Example
Original Circuit
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Thevenin’s theorem can be used to replace any
linear circuit with an equivalent voltage source
called VTH and an equivalent resistance called RTH.
6 kW
72 V
4 kW
3 kW
RR
LV
THTH
Remove
the
load.the open terminals.
Remove
Calculate
the
or
source.
measure
Calculate or measure
VTH
across
Thevenin’s resistance (RTH)
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Thevenin’s Voltage
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Voltmeter Tip
The input impedance of
a voltmeter should be at least 100 times
greater than the Thevenin resistance to
avoid meter loading.
Meter loading errors cause
inaccurate measurements.
DMMs are usually not a problem since they
typically have an input impedance
of 10 MW.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Thevenin Equivalent Circuit
6 kW
Original
circuit
72 V
4 kW
3 kW
RL
6 kW (RTH)
Thevenin
equivalent circuit
24 V (VTH)
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
RL
Norton’s Theorem
Used to replace any linear circuit with an
equivalent current source called IN and an
equivalent resistance called RN
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Norton’s Resistance
6 kW
72 V
4 kW
3 kW
RL IR
NN
RShort
N is the
TH. I .
thesame
load as
to R
find
N
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Norton’s Current
IN = 4 mA
RN = 6 KW
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Norton Equivalent Circuit
6 kW
The original
circuit
The Norton
equivalent circuit
72 V
4 mA (IN)
4 kW
3 kW
RL
6 kW (RN)
RL
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
6 kW (RTH)
A Thevenin
equivalent circuit
Circuit Conversion
The Norton
dual
RL
24 V (VTH)
RN = RTH
4 mA (IN)
IN =
VTH
RTH
6 kW (RN)
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
RL
Solder and Connector Problems
• A solder bridge between two lines
effectively shorts them together.
• A cold solder joint is effectively an open
circuit.
• An intermittent trouble is one that
appears and disappears (could be a cold
solder joint or a loose connection).
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Troubleshooting
• Finding out why a circuit is not doing
what it is supposed to do
• Common problems are opens and shorts
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
An open device
• The current through it is zero.
• The voltage across it is unknown.
• V = zero x infinity {indeterminate}
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
A shorted device
• The voltage across it is zero.
• The current through it is unknown.
• I = 0/infinity {indeterminate}
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
A troubleshooting example:
Do the two 10 W resistors form
a stiff voltage divider?
10 W
12 V
100 kW
10 W
100 kW
Why?
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
A troubleshooting example:
What are the expected
voltages in this circuit?
10 W
12 V
100 kW
10 W
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
100 kW
A troubleshooting example:
What are some causes for
this voltage (V) being too high?
10 W
12 V
100 kW
10 W
100 kW
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
V
A troubleshooting example:
What are some causes for
this voltage (V) being too low?
10 W
12 V
100 kW
10 W
100 kW
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
V