electronic instrumentation 1 experiment 9 part a: simulation of a transformer part b: making an...
Post on 20-Dec-2015
224 views
TRANSCRIPT
1
Electronic InstrumentationExperiment 9
•Part A: Simulation of a Transformer•Part B: Making an Inductor•Part C: Measurement of Inductance•Part D: Making a Transformer
18 October 2003 Electronic Instrumentation 2
Inductors & Transformers
How do transformers work? How to make an inductor? How to measure inductance? How to make a transformer?
?
18 October 2003 Electronic Instrumentation 4
Some Interesting Inductors
Induction Heating in Aerospace
18 October 2003 Electronic Instrumentation 6
Some Interesting Inductors
Coin Flipper
Primary
Coil
Secondary
Coil
18 October 2003 Electronic Instrumentation 10
Some Interesting Transformers
High Temperature Superconducting Transformer
18 October 2003 Electronic Instrumentation 11
Household Power
7200V transformed to 240V for household use
18 October 2003 Electronic Instrumentation 12
Inductors-Review
General form of I-V relationship
For steady-state sine wave excitation
V Ld I
d t
V j L I Z j LL
18 October 2003 Electronic Instrumentation 13
Inductors-Review
Simple R-L Filter• High Pass Filter• Corner Frequency
R2
1k
0
V VL1
1mH
R1
50
V1
FREQ = 1kVAMPL = 1VOFF = 0
fR
LkH z
1
21 6 7
18 October 2003 Electronic Instrumentation 14
Inductors-Review
Frequency
1.0Hz 10Hz 100Hz 1.0KHz 10KHz 100KHz 1.0MHz 10MHz 100MHzV(R1:2) V(L1:1)
0V
0.2V
0.4V
0.6V
0.8V
1.0V
18 October 2003 Electronic Instrumentation 15
Making an Inductor
For a simple cylindrical inductor (called a solenoid), we wind N turns of wire around a cylindrical form. The inductance is ideally given by
where this expression only holds when the length d is very much greater than the diameter 2rc
Henriesd
rNL c )( 22
0
18 October 2003 Electronic Instrumentation 16
Making an Inductor
Note that the constant o = 4 x 10-7 H/m is
required to have inductance in Henries (named after Joseph Henry of Albany)
For magnetic materials, we use instead, which can typically be 105 times larger for materials like iron
is called the permeability
18 October 2003 Electronic Instrumentation 17
Some Typical Permeabilities
Air 1.257x10-6 H/m Ferrite U M33 9.42x10-4 H/m Nickel 7.54x10-4 H/m Iron 6.28x10-3 H/m Ferrite T38 1.26x10-2 H/m Silicon GO steel 5.03x10-2 H/m supermalloy 1.26 H/m
18 October 2003 Electronic Instrumentation 18
Making an Inductor
If the coil length is much small than the diameter (rw is the wire radius)
Such a coil is used in the metal detector at the right
}2)8
{ln(2 w
cc r
rrNL
18 October 2003 Electronic Instrumentation 19
Making an Inductor
All wires have some finite resistance. Much of the time, this resistance is negligible when compared with other circuit components.
Resistance of a wire is given by
l is the wire length
A is the wire cross sectional area (rw2)
is the wire conductivity
A
lR
18 October 2003 Electronic Instrumentation 20
Some Typical Conductivities
Silver 6.17x107 Siemens/m Copper 5.8x107 S/m Aluminum 3.72x107 S/m Iron 1x107 S/m Sea Water 5 S/m Fresh Water 25x10-6 S/m Teflon 1x10-20 S/m
18 October 2003 Electronic Instrumentation 21
Wire Resistance
Using the Megaconverter at http://www.megaconverter.com/Mega2/
(see course website)
18 October 2003 Electronic Instrumentation 22
Transformers
Note that for a transformer, the symbol shows two inductors. One is the primary (source end) and one is the secondary (load end): LS & LL
The inductors work as expected, but they also couple to one another through their mutual inductance: M2=k2 LS LL
Symbol for transformer
18 October 2003 Electronic Instrumentation 23
Transformers
Let the current through the primary be Let the current through the secondary be The voltage across the primary inductor is
The voltage across the secondary inductor is
I S
I L
j L I j M IS L
j L I j M IL S
IS IL
Note Current Direction
18 October 2003 Electronic Instrumentation 24
Transformers
Sum of primary voltages must equal the source
Sum of secondary voltages must equal zero
V R I j L I j M IS S S S S L
0 R I j L I j M IL L L L S
18 October 2003 Electronic Instrumentation 25
Transformers
Note the following simplifying information for cylindrical or toroidal inductors
For k 1
L a LL S 2 a NN
L
S
Henriesd
rNL c )( 22
0
M L L a L LaS L S
L 2 22
2
18 October 2003 Electronic Instrumentation 28
Transformers
Transformers are designed so that the inductive impedances are much larger than any resistance in the circuit. Then, from the second loop equation
Z j LL
0 R I j L I j M IL L L L S
j L I j M IL L S N I N IL L S S
18 October 2003 Electronic Instrumentation 29
Transformers
The voltages across the primary and secondary terminals of the transformer are related by
Note that the coil with more turns has the larger voltage
N V N VS L L S
18 October 2003 Electronic Instrumentation 30
Transformers
The input impedance of the primary winding reflects the load impedance. It can be determined from the loop equations
Z VI R j L L L
R j LINS
SS S
S L
L L
2
Z NN RIN
S
LL
2
18 October 2003 Electronic Instrumentation 31
Transformer Rectifier
Adding a full wave rectifier to the transformer makes a low voltage DC power supply, like the wall warts used on most of the electronics we buy these days.
D2
D1N4148
V
0
V1
FREQ = 60VAMPL = 120VOFF = 0
R1
5
TX1
D4
D1N4148
0
R2
1k
D3
D1N4148
D1
D1N4148C2
33uF
V
18 October 2003 Electronic Instrumentation 32
Transformer Rectifier
Time
10.000s 10.005s 10.010s 10.015s 10.020s 10.025s 10.030s 10.035s 10.040s 10.045s 10.050sV(R1:2) V(R3:2) V(D2:2) V(R4:1)
-120V
-80V
-40V
-0V
40V
80V
120V
Filtered
Unfiltered
18 October 2003 Electronic Instrumentation 33
Determining Inductance Calculate it from dimensions and material
properties Measure using commercial bridge (expensive
device) Infer inductance from response of a circuit.
This latter approach is the cheapest and usually the simplest to apply. Most of the time, we can determine circuit parameters from circuit performance.
18 October 2003 Electronic Instrumentation 34
Determining Inductance
For this circuit, a resonance should occur for the parallel combination of the unknown inductor and the known capacitor. If we find this frequency, we can find the inductance.
18 October 2003 Electronic Instrumentation 35
Determining Inductance
Reminder—The parallel combination of L and C goes to infinity at resonance.
Zj L j C
j L j C
j L
L C||
1
1 1 2
LCf
LC
211
00
18 October 2003 Electronic Instrumentation 36
R1
50 C1
.68uF
V1
FREQ = 1kVAMPL = 1VOFF = 0
V
0
L1
100uH
R2
50
V
Frequency
1.0KHz 3.0KHz 10KHz 30KHz 100KHz 300KHz 1.0MHzV(C1:1) V(C1:2)
0V
0.2V
0.4V
0.6V
0.8V
1.0V
18 October 2003 Electronic Instrumentation 37
Even 1 ohm of resistance in the coil can spoil this response somewhat
Frequency
1.0KHz 3.0KHz 10KHz 30KHz 100KHz 300KHz 1.0MHzV(C1:1) V(C1:2)
0V
0.5V
1.0V
V(R3:2) V(R4:1)0V
0.5V
1.0V
SEL>>
18 October 2003 Electronic Instrumentation 38
Project 3: Beakman’s Motor
The coil in this motor can be characterized in the same way