design realization lecture 14 john canny/dan reznik 10/9/03

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Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

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Page 1: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Design Realization lecture 14

John Canny/Dan Reznik

10/9/03

Page 2: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Last Time

Composites: Fiberglass, carbon fiber and kevlar.

Hierarchical materials.

Cellular materials, honeycomb and foam.

Page 3: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

This time

Electronics

Page 4: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Voltage, Current, Ohm’s law

Voltage is analogous to pressure, and is measured naturally enough, in volts.

Current is analogous to flow, and is measure in amperes or amps for short.

Direct current (DC) is a constant voltage, e.g. a single C or D battery produces 1.5 volts.

Alternating Current (AC) is a voltage that reverse rapidly, at 60 cycles/second in the US. An electrical outlet gives 110 volts AC.

Page 5: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Voltage, Current, Ohm’s law

Resistors are used to produce desired voltage or current, independent of frequency.

Resistance is measured in ohms, and the current through a resistor satisfies Ohm’s law:

V = I R

I in amps

V in volts

Page 6: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Resistors

Resistors have a power rating as well, ½, ¼, 1/8 watt etc. (P = V I)

Resistors used to all look like this:(axial lead type):

But increasingly are surface-mount:

Or grouped in chip packages:

Page 7: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Resistors

Variable resistors are called potentiometers:

Here’s a simple circuit, avoltage divider:

Note the ground and power supply symbols:

A potentiometer can actas a variable voltage divider, to control a voltage.

Page 8: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

AC and frequency

Alternating current most often has a sinusoidal shape over time:

The frequency is thenumber of completecycles per second.

Its measured in Hertz (Hz).

Waveform is

V = sin 2 f t

Page 9: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

AC and Capacitors

Capacitors are charge storage devices, but don’t allow DC to flow.

AC can flow because a little charge is stored each cycle and returned.

The current flow increases with frequency.

Page 10: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Capacitor Construction

Capacitors are sandwiches of dielectric between two conductors.

The dielectric is an insulator, usually a polymer.

Performance determined by “dielectric constant” and electrical breakdown strength (kV/mm).

Page 11: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Capacitor Construction

Page 12: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Capacitor Reactance

A capacitor limits AC current rather like a resistor does.

The reactance Z of the capacitor determines how much current flows, V = Z I where:

C is the capacitance in Farads. A Farad is a huge unit. Most capacitors are

measured in micro-farads or pico-farads (10-12)

CfZ

2

1

Page 13: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Variable Capacitors

Capacitors can be variable. Used for tuning: Radios, antennas, crystal oscillators (to drive

computers).

Page 14: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Inductors

Inductors are coils of wire, sometimes around a ferrite or iron core.

The ferrite core is a composite with small magnetic particles. Works at high frequencies where iron doesn’t.

Page 15: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Transformer

Two coils of wire around the same magnetic core create a transformer.

An AC voltage in one coil induces a voltage in the other.

Ratio of voltages = ratio of turns.

(more turns = highervoltage).

Page 16: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

A simple R/C circuit

This circuit is a voltage divider, with one leg which is a capacitor, one a resistor.

Discuss what “high-pass” and “low-pass” would mean in this circuit.

Page 17: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Amplifiers

Amplifiers are an important class of active component (resistors, capacitors and inductors are passive – they cant strengthen a signal).

Amplifiers boost small signals from radio antennas, microphones, sensors etc. to larger values.

Ex: stereo amplifier. There is a popular component for building

amplifiers called an Operational Amplifier (Op-Amp).

Page 18: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Inverting Amplifier

Here is a basic inverting amplifier. The gain (ratio of Vo to Vi) is - Rf / Ri The OpAmp has very high gain, which makes

it change output until its two inputs are nearly equal – you can assume they are.

Page 19: Design Realization lecture 14 John Canny/Dan Reznik 10/9/03

Non-Inverting Amplifier

Here is a basic non-inverting amplifier. The gain (ratio of Vo to Vi) is (Rf + Rg) / Rg