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Experiment 9 Part A: Simulation of a Transformer

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Presentation on theme: "Experiment 9 Part A: Simulation of a Transformer"— Presentation transcript:

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

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
Primary Coil Secondary Coin Flipper 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 Electronic Instrumentation
Wall Warts 18 October 2003 Electronic Instrumentation

10 Some Interesting Transformers
High Temperature Superconducting Transformer 18 October 2003 Electronic Instrumentation

11 Electronic Instrumentation
Household Power 7200V transformed to 240V for household use 18 October 2003 Electronic Instrumentation

12 Electronic Instrumentation
Inductors-Review General form of I-V relationship For steady-state sine wave excitation 18 October 2003 Electronic Instrumentation

13 Electronic Instrumentation
Inductors-Review Simple R-L Filter High Pass Filter Corner Frequency 18 October 2003 Electronic Instrumentation

14 Electronic Instrumentation
Inductors-Review 18 October 2003 Electronic Instrumentation

15 Electronic Instrumentation
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 18 October 2003 Electronic Instrumentation

16 Electronic Instrumentation
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 x10-6 H/m Ferrite U M x10-4 H/m Nickel x10-4 H/m Iron x10-3 H/m Ferrite T x10-2 H/m Silicon GO steel x10-2 H/m supermalloy 1.26 H/m 18 October 2003 Electronic Instrumentation

18 Electronic Instrumentation
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 18 October 2003 Electronic Instrumentation

19 Electronic Instrumentation
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 (prw2) s is the wire conductivity 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 Electronic Instrumentation
Wire Resistance Using the Megaconverter at (see course website) 18 October 2003 Electronic Instrumentation

22 Electronic Instrumentation
Transformers Symbol for transformer 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 18 October 2003 Electronic Instrumentation

23 Electronic Instrumentation
Transformers IS IL Note Current Direction 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 18 October 2003 Electronic Instrumentation

24 Electronic Instrumentation
Transformers Sum of primary voltages must equal the source Sum of secondary voltages must equal zero 18 October 2003 Electronic Instrumentation

25 Electronic Instrumentation
Transformers Note the following simplifying information for cylindrical or toroidal inductors For 18 October 2003 Electronic Instrumentation

26 Electronic Instrumentation
Transformers Cylinders (solenoids) Toroids 18 October 2003 Electronic Instrumentation

27 Electronic Instrumentation
18 October 2003 Electronic Instrumentation

28 Electronic Instrumentation
Transformers Transformers are designed so that the inductive impedances are much larger than any resistance in the circuit. Then, from the second loop equation 18 October 2003 Electronic Instrumentation

29 Electronic Instrumentation
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 18 October 2003 Electronic Instrumentation

30 Electronic Instrumentation
Transformers The input impedance of the primary winding reflects the load impedance. It can be determined from the loop equations 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. 18 October 2003 Electronic Instrumentation

32 Transformer Rectifier
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. 18 October 2003 Electronic Instrumentation

36 Electronic Instrumentation
18 October 2003 Electronic Instrumentation

37 Electronic Instrumentation
Even 1 ohm of resistance in the coil can spoil this response somewhat 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 18 October 2003 Electronic Instrumentation


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