You electrical engineer types, go take you a free course at MIT.
http://news.yahoo.com/blogs/technolo...225905903.html
You electrical engineer types, go take you a free course at MIT.
http://news.yahoo.com/blogs/technolo...225905903.html
"Friendships come in strange packages
The best ones are opened with a smile"
NA4BH '15
Listened/watched a lot of the lectures on iTunes. Really good stuff.
very interesting.
I AM THE VOICE OF THE VOICELESS!
Calling all Brainiacs?
LIke this?
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If it's a war on drugs, then free the POW's.
So much for that.participants are expected to have a grasp of calculus, linear algebra, and advanced high school level physics.
All the world’s a stage, but obviously the play is unrehearsed and everybody is ad-libbing his lines. Maybe that’s why it’s hard to tell if we’re living in a tragedy or a farce.
Basic Electrical Engineering concepts...
Kirchoff current and voltage laws
1. Sum of voltages in a loop equals 0
2. Sum of currents at a node is 0
1. Voltage Law - Voltage Loop equals 0. Draw a battery with a light bulb across it. Draw the polarities across the battery and light bulb. Starting from the battery positive terminal, in a loop of the battery and light bulb, you have the '+' of the light bulb, then the '-' of the battery. +Vlightbulb - VBattery = 0
Vlightbulb = Vbattery
2. Current Law - Sum of currents at a node is 0. Rewritten, the sum of currents entering a node is equal to currents leaving the node. Example, two resistors tied togther at one end. The tie point is a node. Current flowing through R1 is the same as the current flowing through R2.
Impedance of Resistor is R, resistance.
Impedance of an inductor is Ls, where s = jw, and w = 2(pi)(frequency). Higher the frequency, higher the impedance.
Impedance of a capacitor is 1/(Cs), where s = jw, and w = 2(pi)(frequency). Higher the frequency, lower the impedance
Vout/Vin = Transfer Equation
Suppose we have a resistor between Vin and Vout, and a capacitor from Vout to ground. Vout load is very high impedance, infinite for practical purposes. Current through the resistor is (Vin-Vout)/R. This same current flows through the capacitor, which is Vout/(1/Cs), which also is VoutCs. Current in equals current out, and the load is infinite, so no current flow through Vout. From this we have the equation of current entering the node is equal to current leaving the node. (Vin-Vout)/R = Vout(Cs)
(Vin-Vout)/R = Vout(Cs)
Vin R - Vout R = Vout Cs
Vin R = Vout(R + Cs)
Vin = Vout (R+Cs)/R = Vout (1 + RCs)
Vout/Vin = 1/(1 + RCs), where s = jw = 2(pi)(f)
Decible = 10Log(Vout/Vin)
Corner frequency: -3dB
10 Log(0.5) = -3dB
Vout/Vin = 0.5 = 1/2
At corner frequency, (1 + RCs) = 2, RCs = 1
For RCs = 1, s = 1/RC, 2(pi)f = 1/RC
The corner frequency, fc, is equal to 1/(2RC(pi))
Here, in the equation, Vout/Vin = 1/(1+RCs), where s = 2(pi)f, as f increases, (1 + RCs) also increases, and 1/(1+RCs) will decrease.
This is an example of a low pass filter.