electronic instrumentation 1 experiment 9 part a: simulation of a transformer part b: making an...

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1 Electronic Instrumentation Experiment 9 Part A: Simulation of a Transformer Part B: Making an Inductor Part C: Measurement of Inductance Part D: Making a Transformer

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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 3

Some Interesting Inductors

Induction Heating

18 October 2003 Electronic Instrumentation 4

Some Interesting Inductors

Induction Heating in Aerospace

18 October 2003 Electronic Instrumentation 5

Some Interesting Inductors

Induction Forming

18 October 2003 Electronic Instrumentation 6

Some Interesting Inductors

Coin Flipper

Primary

Coil

Secondary

Coil

18 October 2003 Electronic Instrumentation 7

Some Interesting Inductors

GE Genura Light

18 October 2003 Electronic Instrumentation 8

Some Interesting Transformers

A huge range in sizes

18 October 2003 Electronic Instrumentation 9

Wall Warts

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 26

Transformers

Cylinders (solenoids)

Toroids

18 October 2003 Electronic Instrumentation 27

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

18 October 2003 Electronic Instrumentation 39

Optional Project: Paperclip Launcher

A small disposable flash camera can be used to build a magnetic paperclip launcher