# 1.14 Differentiators  This is an example of a differentiator.  Send a signal in, and the signal you get out will be just the edges of the wave form.    If the input signal is a square wave, then the output will be a series of spikes at each of the sides of the square wave

Incidentally, having a wave that includes spikes could indicate that you have unintentional capacitive coupling.

# 3D printer that can print circuits (\$9,000) The Voxel8 3D printer (www.voxel8.co/) can print cavities to place electronics and components and print conductive material to connect them.  The video from CES will give you an idea of what they can do.  They print a quadcopter frame, pausing to have the controller board, motors, LED inserted in, and print the conductive material to connect them together.  Pretty amazing that it is only \$9,000.

Voxel8 3D printer can print a complete quadcopter, including the circuits

# 1.13 RC circuits: V and I versus time Let’s look at how voltage (V) and current (I) change with respect to time in circuits with capacitors and resistors.

Take a look at this circuit: Close the switch S1 connecting the capacitor (C1) to the battery (Vi) through resistor (R1).  How fast will C1 charge?

That is determined by the relationship between R1 and C1.  It is known as the RC time constant.

Assuming that C1 = 1 microfarad and R1 = 1k ohm, then the time constant will be 1.   And we have a shortcut that it will be within 1% of the input voltage with in 5RC, so within 5 seconds.

# Logging 3 photo-resistors I have three photoresistors in my study that are measuring light coming from 3 directions and showing the live and historical data on the graphs below. How did I do it?

Simple circuit.  Here is how the Arduino is hooked up.  (The resistors are 10k.) /* Simple test of the functionality of the photo resistor

Connect a resistor (around 10k is a good value, higher
values gives higher readings) from pin 0 to GND. (see appendix of arduino notebook page 37 for schematics).

—————————————————-

PhotoR 10K
+5 o—/\/\/–.–/\/\/—o GND
|
Pin 0 o———–

Similar setup for Pin 1 & Pin 2.

—————————————————-
*/

int lightLeftPin= A0;
int lightMidPin =A1;
int lightRightPin = A2;

int lightLeft, lightMid, lightRight;

void setup()
{
Serial.begin(9600); //Begin serial communcation
}

void loop()
{

Serial.println(“###BOD”);
Serial.print(“light_right,”);
Serial.println(lightRight);
Serial.println(“###EOD”);
delay(15000);

Serial.println(“###BOD”);
Serial.print(“light_mid,”);
Serial.println(lightMid);
Serial.println(“###EOD”);

delay(15000);

Serial.println(“###BOD”);
Serial.print(“light_left,”);
Serial.println(lightLeft);
Serial.println(“###EOD”);

delay(15000);
}

I then setup an account at ThingSpeak.com

And to connect the arduino to the internet I used my laptop and a program called Seriot.  It can be downloaded from:

nuewire.com/seriot/

This program will listen to the serial port and write the data to ThingSpeak.com You can then use Restful API calls to get to the data and to chart it.

They have a nice ChartEditor

thingspeak.com/channels/23070/charts/  # 1.12 Capacitors Capacitors hold charge.  Capacitors do not conduct.

We measure capacitance in farads and charge in coulombs (equivalent to the charge 6×10^18 electrons).

a capacitor with 1 farad of capacity will charge 1 coulomb of charge after 1 volt has been applied across its terminals for 1 second.

Q=CV

The capacitor is basically plates of two conductors separated by a non-conductor.  When a voltage is applied, the charge accumulates.  And when the voltage has been removed, then it can release that charge.

I found this really cute video that explains a capacitor:

The total capacitance of capacitors in parallel is the sum of the capacitors.

Ctotal = C1+C2+C3…

Capacitors in parallel will always result in a BIG capacitance.

However capacitors in series will always result in a smaller capacitance.  Two capacitors in series have the capacitance of:

Ctotal = (C1C2)/(C1+C2)

Capacitors in series will always result in a capacitance smaller than the smaller capacitor.

Since capacitors do not conduct current, they do not dissipate power.

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# 1.11 Signal Sources

There are a variety of test equipment that can create signals with ranges of different characteristics.  Three classes of these signal sources we will talk about today: Signal Generators, Pulse Generators, and function Generators.

Signal Generators produce sine waves while allowing you to define the amplitude, frequency, and even allowing for these to vary overtime. Pulse Generators create pulses, allowing for you to vary the amplitude, pulse width, frequency, and even rise time and fall time. Function Generators allow for you to create more complex waves, in a variety of shapes: # 1.09 Other signals and 1.10 Logic Levels Let’s cover two sections today:
1.09 Other signals
1.10 Logic Levels

We have been looking at Voltage as a function of time and seeing how it will look on a graph.  The past few days we have talked about graphs that are sine wave. But there could be other ways that this could look too.  Consider if voltage started out at zero and continued to increase.  It would look something like this: But it is not possible to increase voltage indefinitely and so the graph would really look like this:  (Ramp with limit) But there are other interesting graphs to.  Consider the case of voltage increasing to a point, and then when it reaches a certain point it goes to zero and then begins again.  Let’s say you have a circuit that triggers at a certain voltage, and a capacitor that you are charging up till that point.  It might looks something like this sawtooth wave: But you can also imagine a case where it reaches a point and decreases at the same linear rate.  This would look like a triangle wave: And then there is noise, a complex, background static that we always need to consider and usually minimize: Square waves Steps Spikes But in digital electronics we concern ourselves with logic levels and interrupting a particular voltage as either a true or a false; as a on or a off; as a 1 or 0.  Most digital electronics have a threshold voltage.  Above that voltage it is considered to be true/on/1.  Below that voltage it is considered to be false/off/0. # 1.08 Signal amplitudes and decibels

Peak-to-peak amplitude (pp amplitude) is twice the amplitude. This is the measurement of the amplitude from the bottom peak to the top peak as illustrated below: root-mean-square amplitude (rms amplitude) has different formulas based upon the shape of the signal.  For sine waves only it is given by: Decibels is a comparison between two signals.

When comparing amplitude use this formula: When comparing the power use this formula: Sometimes decibels are presented as units.  This is because their is an implicit signal that is being used for comparison.  Here are some common ones:

a) dBV:  1 volt rms

b) dBm – the voltage corresponding to 1mW with an assumed load impedance

c) small noise generated by a resistor at room temperature

# 1.07 Sinusoidal signals The next few sections in The Arts of Electronics deals with signals.  What are the characteristics of signals?  Amplitude, frequency, shape, etc.

The values we are looking at is voltage as a function of time.  The most basic signal is the sinusoidal signal.  Have you ever graphed y=sin(x) and end up with: But how would you compare this wave to the following:  There are two key things to think about when comparing sine waves:  frequency and amplitude.    The amplitude is the distance from y=0 to the top of the sine wave.  The frequency is how many times the wave repeats in a given period of time.  We typically use the unit hertz (Hz) for frequency, which is one cycle (or period) per second.  Lets take a look at period and amplitude in our original sine graph: The formula that you should remember is

V=A*sin(2*pi*f*t)

A is the amplitude in volts, f is the frequency in Hz and t is the time in seconds.

# 1.06 Small-signal resistance Ohm’s law is R=V/I.  For the ordinary resistance, this is a constant proportion for a large range of V.  But this is not true for all devices.  Today we look at the Zener diode which has a high resistance up to a point and then almost no resistance for a large range of V.  Also, we look at the tunnel diode (also known as the Esaki diode) which actually has a negative resistance over a particular range of V.