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My Study of Inductors or Coils for the VTA/SQM

 


 

 

HI Everyone,

I have done a study of inductors. It is a very complex area to study when one starts from only a basic understanding. I hope I have it all right so please let me know if you see a mistake. First of all when I do a study of something I try to learn as best as possible the terminology. I have compiled a list of definitions of the terms used when working with Inductors. This is a very in depth area and is not easy for a beginner. I am taking small steps. I have started with Impedance because I think this was the hardest to properly understand.

Attribute:

Unit:

Symbol:

Definition:

Impedance:

Ohms

Z

The total opposition to a changing current by an electric circuit, simply put the combination of Reactance and Resistance is known as Impendence. Impendence is not just the arithmetic sum of Reactance and Resistance it is equal to the square root of the sum of the squares of the resistance and reactance of the circuit.

Coil Efficiency:

Nil Q

Sometimes referred to as just Q. This is resonance of the coil at a particular frequency with the exclusion of other frequencies. At a point where the coil reaches it highest efficiency, the value of Q moves toward infinity.

Reactance:

Ohms X

The opposition of inductance and capacitance to alternating current, expressed in ohms: equal to the product of the sine of the angular phase difference between current and voltage and the ratio of the effective voltage to the effective current.

Capacitive Reactance: Nil XC

The opposition of capacitance to alternating current, equal to the reciprocal of the product of the angular frequency of the current times the capacitance.

Inductive Reactance: Nil XL

The opposition of inductance to alternating current, equal to the product of the angular frequency of the current times the self-inductance.

Inductance:

Henry L

That property of a circuit by which a change in current induces, by electromagnetic induction, an electromotive force.  

Inductive Coupling:

Nil  

The coupling between two electric circuits through inductances linked by a common changing magnetic field.

Mutual Inductance:

Henry M

The ratio of the electromotive force in one of two circuits to the rate of change of current in the other circuit.

Self-Inductance: Henry k

Inductance inducing an electromotive force in the same circuit in which the motivating change of current occurs, equal to the number of flux linkages per unit of current.

Distributed Capacitance: Nil C (F/m)

Any capacitance other than that within a capacitor. For example, the capacitance between adjacent turns of wire in a coil.

Resonance: Nil Nil

That condition of a circuit with respect to a given frequency or the like in which the net reactance is zero and the current flow a maximum. Directly related to Q Coil Efficiency.

Flux-Linkage: Maxwell F The rate of cutting of the Magnetic Lines of force by a conductor. Proportional to the rate of change of the Flux moving over the conductor.
Permeability: Henries per Metre (H/m) m Also called magnetic permeability. A measure of the ability of a substance to sustain a magnetic field, equal to the ratio between magnetic flux density and magnetic field strength. For a vacuum, its value is 1.257 × 10-6 henries per meter. Highly magnetisable materials, such as ferromagnetic materials, have higher magnetic permeability.
Former: Nil Nil Formers are the devices the coils are actually wound. They are made of Insulating materials such of ceramic, paxolin, ebonite, plastic's or cardboard.
Magnetic Flux : Oerstead H Φ or H is the magnetic field strength due to a current flowing in a coil. The mmf is the force caused by a current I flowing through N turns. In a coil it is the total current linked with the magnetic circuit. The SI unit of magnetic flux is the weber (in derived units: volt-seconds), and the unit of magnetic field is the weber per square meter, or tesla.
Weber: Nil Nil The weber may be defined in terms of Faraday's law, which relates a changing magnetic flux through a loop to the electric field around the loop. A change in flux of one weber per second will induce an electromotive force of one volt.
Magnetomotive force: Tesla At The standard definition of magnetomotive force involves current passing through an electrical conductor, which accounts for the magnetic fields of electromagnets. Permanent magnets also exhibit magnetomotive force, but for different reasons. Measured in the ampere-turn (AT).
Ampere-Turn: Nil At The ampere-turn (AT) is the MKS unit of magnetomotive force, represented by a direct current of one ampere flowing in a single-turn loop in a vacuum. "Turns" refers to the winding number of an electrical conductor comprising an inductor. An ampere-turn is equal to 4 Π/10 gilberts, the equivalent CGS unit.
Gilbert: Nil Gi The gilbert, established by the IEC in 1930, is the CGS unit of magnetomotive force. The gilbert is defined differently, and is a slightly smaller unit than the ampere-turn. The unit is named after William Gilbert.
Gauss: Nil Nil  Abbreviated as G, is the cgs unit of magnetic flux density in a magnetic field (B), named after the German mathematician and physicist Carl Friedrich Gauss. One gauss is defined as one maxwell per square centimetre.
Gauss' law: Nil Nil Gauss' law is a law relating the distribution of electric charge to the resulting electric field. It is one of the four Maxwell's equations, which form the basis of classical electrodynamics, and is also closely related to Coulomb's law.
Gauss's law for magnetism: Nil Nil Gauss's law for magnetism is one of the four Maxwell's equations which underlie classical electrodynamics. It states that the magnetic field B has divergence equal to zero, in other words, that it is a solenoidal vector field. It is equivalent to the statement that magnetic monopoles do not exist. Rather than "magnetic charges", the basic entity for magnetism is the magnetic dipole.
Electric displacement field: Nil D The electric displacement field is a vector field that appears in Maxwell's equations. It accounts for the effects of bound charges within materials. "D" stands for "displacement," as in the related concept of displacement current in dielectrics.
Electric field: Nil E The space surrounding an electric charge or in the presence of a time-varying magnetic field has a property called an electric field (that can also be equated to electric flux density). This electric field exerts a force on other electrically charged objects.
Electric Charge: Nil q Electric charge is a fundamental conserved property of some subatomic particles, which determines their electromagnetic interaction. Electrically charged matter is influenced by, and produces, electromagnetic fields.
Phase: Nil Nil When there exists a time interval in the starting point of two alternating currents or Voltages we say there exists a Phase difference between the two wave forms.
Phases of Current and Voltage in a Coil and Capacity: Nil Nil It can be shown Mathematically and in the Lab that current through an inductor (Coil) lags behind the Applied Voltage by 90o and the current in a capacitor leads over the applied Voltage by 90o
Frequency: Hertz Hz Frequency is a measure of the number of occurrences of a repeating event per unit time.
Duty Cycle: Nil D Duty cycle is the proportion of time during which a component, device, or system is operated. Suppose a disk drive operates for 1 second, and is shut off for 99 seconds, then is run for 1 second again, and so on. The drive runs for one out of 100 seconds, or 1/100 of the time, and its duty cycle is therefore 1/100, or 1 percent.
Pulse-width modulation: Nil Nil Pulse-width modulation (PWM) of a signal or power source involves the modulation of its duty cycle, to either convey information over a communications channel or control the amount of power sent to a load.

I could add much more to the above table but this should suffice for what I am trying to achieve. Many references from Wikipedia. As you can see there is a lot of complex information when working with a coil of wire if one is trying to get good results. A good example of high Q (Coil Efficiency) is John Bedini's SG Motor. In this motor John has shown resonance points when it is starting. It can be seen on the Amp meter when starting the motor.

Ohms Law.

This is very important to know about before even starting work on the building of inductors. Ohms law will be familiar to many but I am going over it again for those that do not know. Ohms Law is the holy grail for Electric circuits. Ohms law defines the relationships between Power (P), Current (I), Voltage (E) and Resistance (R). The Equations are as follows:

Power

P = I 2 x R

P = E x I

P = E 2 / R

 

Current

I = P / E

I = P/R

I = E / R

 

Voltage

E = I x R

E = P / I

E = PxR

 

Resistance

R = P / I 2

R = E / I

R = E 2 / P

 

Power is measured in Watts. One familiar use Kilo Watt Hours displayed on the electricity bill, or "the motor is a 1.8Kw Motor". The power we use is determined by these units. Current is measured in Amperes, or depending on what one is doing Micro, or Mill Amperes. I can illustrate this much better with a diagram:

Above we can see, I = E / R.

1/1 = 1 so I = 1

A is an Amp Meter and we see the current in the simulation is 989.11mA, it would be 1 Ampere but there are small losses in the circuit. This illustrates the calculation from simple circuit components and can be substituted for other parts. There are many good Ohms Law calculators on the net. This one is one I like: Click Here.

Now I could ramble on for many hours but that is outright boring. I am sure a better way is to watch some VERY Good videos about Inductors and Coils by a true professional. There is a very good series of Video Lecture's on Inductors: Click Here. Walter Lewin is the Physics Professor that is giving these lectures. He does an excellent job. I would love to have this man in my lab every time I have a problem to help me work it out. I can HIGHLY recommend watching the following list.

Lecture #2:

Electric Field
Field Lines
Superposition
Inductive Charging
Dipoles
Induced Dipoles

Lecture #3: 

Electric Flux
Gauss's

Lecture #9:


Currents
Resistivity
Ohm's Law

 

Lecture #11:

Magnetic field
Lorentz Force
Torques
Electric Motors (DC)
Oscilloscope

 

Lecture #15:

Ampere's Law
Solenoids
Revisit the Kelvin

 

Lecture #16:

Electromagnetic Induction
Faraday's Law
Lenz Law
Complete Breakdown of Intuition
Non-Conservative Fields

 

Lecture #17:

Motional EMF
Dynamos
Eddy Currents
Magnetic Braking

Lecture #20

Inductance
RL Circuits
Magnetic Field Energy

Lecture #22:

Hysteresis
Electromagnets
Bohr Magneton

 

Lecture #24:

Transformers
Car Coils
RC Circuits

 

Lecture #25:

Driven LRC Circuits
Resonance
Metal Detectors (Beach/Airport)

 

Lecture #27:

Resonance
Destructive Resonance
Electromagnetic Waves
Speed of Light
Radio - TV
Distance Determinations using Radar and Lasers

 

You can download the streaming video files if you prefer to play these files off-line. MIT OpenCourseWare video files stored on the Akamai network will have two types of URLs. There are video and audio only URLs (RealMedia files only), and URLs for video and audio files that have supporting files such as captioning (RealMedia with supporting files).

RealMedia Files Only
If the URL looks like http://mfile.akamai.com/7870/rm/mitstorage.download.akamai.com/ 7870/18/18.06/videolectures/strang-1806-lec01-26aug1999-220k.rm, you can download using these instructions:

  • You can find the URL for the video you want by right-clicking on the link and selecting "Copy Link Location…" (ctrl-click on a Mac).

  • Remove the entire first part of the URL:
    http://mfile.akamai.com/7870/rm/mitstorage.download.akamai.com/7870

  • Add http://ocw.mit.edu/ans7870 instead. This will be the link to download the RealMedia file. It will look something like this:
    http://ocw.mit.edu/ans7870/18/18.06/videolectures/strang-1806-lec01-26aug1999-220k.rm

  • Make sure you Save the file to a convenient location like your Documents or Video folder.

These lectures are absolutely brilliant videos and anyone wanting to learn more about coils these are a must see. I very much wish more excellent content like this was more freely distributed on the net. Thank you MIT and very big thank you Walter Lewin. Great job.

Inductance and Generating currents.

It is important to note that (Flux Cutting), I like to use Flux Modulation, in a generator is dependent on a few different things. First we have a look at Nikola Tesla's Polyphase Generator:

Tesla's Polyphase Alternating Current 500 horse power generator.

The Cross Sectional Area of the inductor is important for the output. This is also true for transformers. The Flux lines of the Magnet per Unit Area are different for mild strength or high strength magnets. High Strength Magnets have closer flux lines compared to wider apart Flux lines of a mild strength magnet. To induce large currents, a fairly large inductor will be needed dependent on the Magnetic Flux Strength of the Magnet, referred to Magnetic Flux Density. This is visible in the above Generators or Dynamo's.

Calculations follow the following formulas:

H is flux density and is considered, in transformers, to be 60,000 Lines of magnetic Flux per square inch.

N = 100000000/4.44 x F x 60,000 x A

N = Number of turns. A = Cross Sectional Area of Winding of Form. F = Frequency of modulation. So an Example would follow as such. We are looking for the number of turns.

N = 100000000/4.44 x 60 x 60,000 x 3.43 = 2 turns per volt. So 240 turns for 120 volts and 480 turns for 240 volts.

You can see here that we need a big cross sectional Area of the inductors to get the desired result for 120 volts. I have played with small inductors and failed. The turn Ratio/Area is needed for overall Inductance or there will be no or a very poor result. Although this is a reasonably big cross sectional area it is well beyond an achievable result for the VTA/SQM/ A Transformer with a centre core Area of 2 Inches by 1.5 will fit the bill here quite easily and they are easy to come by.

Now as you can see, if there was two main coils in between the magnets there would be no room for the other coils. You would be right. This version of the VTA/SQM had no Quadrature coils and we can see from the below Schematic there was a Transformer doing the job of the Quadrature Coils. In the next Picture we can see there was Quadrature Coils and there is a Transformer, from the VTA Video we know this Transformer was a step down Transformer to power the 12V Lights and Motor. However we can not easily see the battery to start the VTA/SQM as we could see in the last picture (Top Right Hand Corner). Again even more proof to show there was no conditioning of the magnets prior to the Magnets being introduced to the VTA.

The VTA/SQM is a steady State Alternator. Better put a Space Quanta Modulator. Read the Nothing is Somthing Document and it will answer most of your questions. Don't wait for these many of hundreds of companies that make broken promises and NEVER deliver. Do it for yourself.

Some more good reference material I can recommend is: Click Here

I like to check Tom Bearden's Website for terms and definitions also when something does not make allot of sense: Click Here

 

Well more coming soon as always.

_____________________
To reach new horizons...

   
 

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