Vocademy - Electronics Technology
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updated 1 year ago
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
This is a remake of the previous video by the same name but I added several clarifying graphics.
Refractive Optics:
youtu.be/qDGU71FQ878
Reflective Optics:
youtu.be/jV5EtWbYIlo
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Help make these videos and keep Vocademy free:
patreon.com/vocademy
paypal.me/VocEd
My astronomy site:
amsky.net
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Actually, accepted classical and relativistic physics can explain this force. This video explains my take on it.
Here are the other videos mentioned in this video:
EtherealMechanics - Science is broken:
youtu.be/5BRvwhfdfVg
Vocademy - Electricity, Magnetism and Special Relativity:
youtu.be/Z31jsD63nsA
Veritasium - How Special Relativity Makes Magnets Work
youtu.be/1TKSfAkWWN0
Fermilab - Dr. Don Lincoln - How Einstein saved magnet theory
youtu.be/d29cETVUk-0
To support free vocational education at Vocademy and this channel, go to patreon.com/vocademy
Vocademy - Free Vocational Education
The thumbnail for this video shows an ultraviolet laser beam coming from the adaptive optics system of the 60-inch (1.5 meter) telescope on Palomar Mountain. The laser creates an artificial star that the adaptive optics system uses to continually align the system to eliminate atmospheric turbulence. The beam is UV (invisible to the eye), but the image was taken with a DSLR camera that had the UV filter removed. The UV light stimulates the RGB sensors to different amounts, resulting in a false orange appearance.
Vocademy - Free Vocational Education
The nature of light, part 2. Interference, diffraction, refraction and reflection.
The wave/particle duality of light, wavelength, frequency, phase, and polarization.
What are loudspeakers, and how are speaker enclosures made.
The nature of sound
Using microphones
A Quick Look at Decibels:
youtu.be/aiEI8KiuVT8
This video discusses the development and types of microphones.
Revisiting the variable duty cycle op-amp-based relaxation oscillator with the Falstad circuit simulator.
Errata:
I misread the oscilloscope trace I used to show the voltages and currents of the charastic curve of a tunnel diode--I misread by a factor of 10, seeing 8 mA as 80 mA. This throws off my current and impedance numbers by the same factor. This doesn't affect the explanation and would be correct for a tunnel diode that operates at the currents I mentioned. However, it turns out that the curve I misread is typical, making my numbers unrealistic. While relating this video to a real tunnel diode, decrease the currents by a factor of 10 and increase the impedances/resistances by the same factor.
Circuit simulator at falstad.com:
Tunnel Diode Relaxation Oscillator:
falstad.com/circuit/e-tdrelax.html
Click Circuits, Misc Devices, Tunnel Diodes, and LC Oscillator for the LC tunnel diode oscillator.
Yes, I was quoting Peter Schickele at the conclusion of the video.
The Clapp, Vackář, and Seiler oscillators are based on the Colpitts oscillator.
The Clapp oscillator adds a variable capacitor in the inductor leg of the tank circuit. This capacitor is typically about one-tenth of the combined capacitance of the two capacitors on the other leg of the tank circuit. Having a lower capacitance gives the variable capacitor a greater effect on the frequency (lower capacitance causes higher capacitive reactance).
The Vackář oscillator moves the inductor out of the tank circuit and closer to the transistor's collector. This gives the Vackář oscillator greater frequency and voltage stability.
The Seiler oscillator uses a capacitor network to provide positive feedback from the emitter to the base of the transistor.
Errata:
I misread the oscilloscope trace I used to show the voltages and currents of the charastic curve of a tunnel diode--I misread by a factor of 10, seeing 8 mA as 80 mA. This throws off my current and impedance numbers by the same factor. This doesn't affect the explanation and would be correct for a tunnel diode that operates at the currents I mentioned. However, it turns out that the curve I misread is typical, making my numbers unrealistic. While relating this video to a real tunnel diode, decrease the currents by a factor of 10 and increase the impedances/resistances by the same factor.
The quantum tunneling effect causes a tunnel diode to act much like a fixed resistor of about five or six ohms when reverse-biased or below about 50 millivolts when forward-biased. Between about 50 millivolts and 300 millivolts (0.05 and 0.3 volts), assuming a germanium diode, the impedance of the tunnel diode increases exponentially as the voltage increases. This causes the current to decrease linearly as the voltage increases; the reverse of a fixed resistor. This is called the negative resistance region. Above 300 millivolts, the germanium tunnel diode acts like a regular germanium diode.
The negative resistance region, along with the tunnel diode's low capacitance, can be exploited to create microwave-frequency oscillators. The tunnel diode acts like a voltage-sensitive variable resistor that provides a current inverse to the voltage of a ringing tank circuit. This current is, thus, fed into the tank circuit at the correct phase to compensate for the damping as energy is dissipated by the circuit's resistance.
The "little green man" model used in this video is similar to the LGM model I use to explain the zener diode in the following video: youtu.be/RSHahPnioW0
The blocking oscillator exploits circuit saturation to cause a sudden collapse of the magnetic field in the primary of a feedback transformer. This sudden collapse of the magnetic field causes the transistor base voltage to drop or reverse, blocking the transistor's operation. This desaturates the circuit and starts the cycle over.
Relaxation oscillators exploit a sudden change in a circuit parameter when the circuit reaches a given voltage or current. This change does not reverse until a different threshold is reached (hysteresis). In the simplest example in this video, a neon light starts to conduct when a parallel capacitor charges to about 90 volts. The conducting bulb discharges the capacitor. The bulb stops conducting at around 60 volts, allowing the capacitor to charge again. Other relaxation oscillators use different mechanisms, but the common characteristic is one voltage of current triggering a change in the circuit but a different voltage or current reversing the change.
youtu.be/cwY2AOUhtLM
The transistor symbol in the schematic for a Pierce oscillator is for a PNP transistor where the 2N2222 and 2N3904 are NPN transistors. There is a link to the corrected schematic at the appropriate point in the video and here: youtu.be/SQ9_buobb9M
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Vocademy - Free Vocational Education
Here is the link to my detailed video on the astable multivibrator:
youtu.be/9eRWKh7OOHw
Vocademy - Free Vocational Education
Learn More:
How FOUCAULT PENDULUM Works...:
youtu.be/8JxyT0edT6c
What the Phugoid is... (I need to make a minor correction):
youtu.be/9DnSG4H2UjE?
How to get feedback out of choir mics:
youtube.com/live/FoZoZv9IY1Q
Escapement Theory:
youtu.be/SUuv0_gHQQs
Vocademy - Free Vocational Education
00:00 Title and introduction
01:11 What is oscillation
06:40 What are oscillators
08:49 Key requirements
11:54 Sine waves and harmonics
20:20 Feedback in an auditorium
29:33 The phase shift oscillator
40:10 Coming up
40:34 Epilog
I am preparing to do a video series on oscillators. Here is a short preview of where this is taking me.
Learn electronics technology for free at vocademy.net
Solid-state Devices and Analog Circuits
Day 6, Part 2
Practical Analog Circuits
Solid-state Devices and Analog Circuits
Day 6, Part 1
Math Review
Exponents and Logarithms
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Solid-state Devices and Analog Circuits - Day 9 Supplemental
While working on my laser communicator, my power supply failed, and not failing to a safe condition, it put 23 volts across my laser pointer. Let's see what happened.
The J-FET is a modification of the diode. By manipulating the width of the depletion region, by changing the gate-to-source voltage, the conductance between the drain and the source is changed.
Reading assignment:
http://vocademy.net/textbooks/solidstatedevices/ShowPage.php?CourseDirectory=solidstatedevices&FileName=FieldEffectTransistors
Here's the playlist for this lecture series:
youtube.com/playlist?list=PLNm1_xEfhzSCIJuy-pBP7fZvwjRPXrp5C
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MOSFETs are a very popular transistor because of their low power consumption. This video explains their basic operation.
Reading assignment: http://vocademy.net/textbooks/solidstatedevices/ShowPage.php?CourseDirectory=solidstatedevices&FileName=FieldEffectTransistors
Here's the playlist for this lecture series:
youtube.com/playlist?list=PLNm1_xEfhzSCIJuy-pBP7fZvwjRPXrp5C
Learn electronics technology for free at Vocademy -- vocademy.net
vocademy.net
Inverted Realities (youtu.be/ldjIkYqV9xo) tested Dr. Walter Lewin's hypothesis using a toroidal inductor. He didn't take into account that emf acts as if it only exists inside the toroid hole and concluded that Kirchhoff's Voltage Law fails with a changing magnetic field. Applying the nature of a toroidal inductor and Kirchhoff's Voltage Law, I predicted Inverted Realities' outcome. This shows that by understanding how devices work, you can make accurate predictions and not be fooled by false premises.
Here are the videos referred to in this video:
Kirchhoff's Voltage Law Fails, or Does it: youtu.be/jHTT-m4_F4o
Where is the emf in a Toroidal Inductor: youtu.be/WLwoc43Foeo
Voltage in a Loop is Weird: youtu.be/Bp3iw_tBdvQ
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Amplifiers are classified according to how many degrees of a sine wave they operate on.
Video on switching regulators: youtu.be/86E3ONEJXbY
Switching regulators are more efficient than linear regulators.
Class B push-pull amplifiers are more efficient than Class A amplifiers.


