electrical-polarization-process.pdf

Polarization in a Water Capacitor
The Fermi Level Barrier
Ionization of the Water Molecule
The Dielectric Constant of Water
Hydrogen Bonds
Pulse Period Manipulation and Polarization
Molecule & Gas Atom Ionization - Raising H+ to 13.6 electronVolts
Voltage Threshold & Amp Restriction Levels
Electrical
Polarization Process

A capacitor is a device that stores electrical energy in an electric field by separating charges on
two conductive plates that are separated by a non-conductive material called a dielectric. In the
case of a water-filled capacitor with two tubular plates, the dielectric is the water itself. This type of
capacitor is called an electrolytic capacitor, and it has some unique properties due to the
polarization of the water molecule.
The water molecule is a polar molecule, meaning that it has a positive charge on one end and a
negative charge on the other. This polarization is due to the unequal distribution of electrons in the
molecule, which causes the oxygen atom to have a slight negative charge and the hydrogen atoms
to have a slight positive charge. When a voltage is applied to the two tubular plates in the water-
filled capacitor, the polar water molecules align themselves with the electric field, with the positive
ends of the molecules facing the negative plate and the negative ends facing the positive plate.
This causes a separation of charge in the water, with the positive ions accumulating near the
negative plate and the negative ions near the positive plate.
The 304L stainless tubing used in the water-filled capacitor is a good conductor of electricity, but it
has a relatively low breakdown voltage. This means that if the voltage across the capacitor
exceeds a certain threshold, the tubing can break down and become damaged. To increase the
voltage threshold of the capacitor, the tubing can be doped with Cr2O3, which is a ceramic
material that has a high dielectric strength. When the tubing is doped with Cr2O3, it becomes a
better insulator and can withstand higher voltages without breaking down.
Polarization in a Water
Capacitor
The dielectric constant of a material is a measure of how easily it becomes polarized in
an electric field. The dielectric constant of water is relatively high, which means that it is
easily polarized by an applied electric field. This makes water a good dielectric material
for use in electrolytic capacitors.

In summary, the electrical polarization of the water molecule in a water-filled capacitor with
two tubular plates is an important factor in the capacitor's performance. The high dielectric
constant of water allows for efficient energy storage, while the use of Cr2O3-doped 304L
stainless tubing can increase the voltage threshold of the capacitor and prevent damage due
to breakdown.

The Fermi level is a
concept used in solid-state physics to describe the energy level at which electrons in a material
have a 50% probability of being occupied. In the case of natural water and a 304L stainless steel
electrode, the behavior of the Fermi level is important in understanding the electrochemical
reactions that occur at the electrode-water interface.
Natural water, such as that found in lakes, rivers, and oceans, is a complex mixture of dissolved
gases, ions, and organic compounds. These components can interact with the electrons in the
water and affect the position of the Fermi level. The Fermi level of natural water is generally close
to the energy level of the water's highest occupied molecular orbital (HOMO), which is the energy
level of the highest occupied electrons in the water molecule.
304L stainless steel is a commonly used material for electrodes in electrochemical applications due
to its excellent corrosion resistance and durability. The Fermi level of the metal can be affected by
several factors, including the presence of impurities, defects, or surface treatments. In the absence
of any external influences, the Fermi level of 304L stainless steel is typically located within the
energy band gap of the material.
When a 304L stainless steel electrode is submerged in natural water, electrochemical reactions can
occur at the electrode-water interface. These reactions involve the transfer of electrons between
the electrode and the water, which can cause changes in the position of the Fermi level. If the
electrode is more electronegative than the water, electrons will flow from the water to the
electrode, causing the Fermi level of the water to decrease and the Fermi level of the electrode to
increase. This can result in the formation of an electric double layer at the electrode-water
interface, which can affect the behavior of ions and molecules in the water.
The Fermi Level Barrier

The behavior of the Fermi level of
natural water and a 304L stainless steel electrode is important in many electrochemical
applications, including corrosion prevention, electroplating, and water treatment.
Understanding the electrochemical reactions that occur at the electrode-water interface can help to
optimize these processes and improve their efficiency and effectiveness.
The position of the Fermi level can be affected by several factors, including the composition of the
water, the surface condition of the electrode, and the electrochemical reactions that occur at the
electrode-water interface. By understanding these factors, researchers and engineers can develop
new and improved methods for electrochemical applications.
The Schottky diode is a semiconductor device that has revolutionized electronics since its
discovery in the early 20th century. It is named after the German physicist Walter H. Schottky who
first observed the phenomenon of rectification in metal-semiconductor junctions in 1938. Schottky
diodes are used in a wide range of electronic applications, from power conversion to radio
frequency signal detection.
The basic principle behind the Schottky diode is the manipulation of the Fermi level of a
semiconductor by the introduction of a metal layer. When a metal is deposited on a semiconductor
material, it forms a junction that allows current to flow in only one direction. The metal-
semiconductor junction behaves like a diode, allowing current to flow in only one direction, from
the metal to the semiconductor.
See Stephen Meyer's Radio Interviews for his unique perspective on the birth of the
Schottkey diode, the behavior of the P-metal junction and how natural water introduces a
doping effect on the SS 304L capacitor plate.
"Don't ask, what the metal electrode introduces to the water. Ask, what the water introduces
to the metal electrode."
~ Stephen Meyer

The Schottky diode is different from a conventional p-n junction diode in that it has a metal-
semiconductor junction, rather than a p-type and n-type semiconductor junction. The metal
layer in the Schottky diode is typically made of a noble metal such as gold, platinum, or tungsten.
The semiconductor material can be either p-type or n-type. The metal layer is deposited onto the
semiconductor material through a process known as sputtering.
Schottky diodes have several advantages over p-n junction diodes. They have a lower forward
voltage drop, faster switching speed, and lower reverse recovery time. These properties make
them ideal for high-frequency applications such as radio frequency detection and power
conversion.
Experiments with P-metal and N-metal junctions have shown that doping can create either a
resistive-like connection or a diode-like connection. Doping is the process of introducing impurities
into a semiconductor material to alter its electrical properties. In p-type semiconductors, the
doping introduces acceptor impurities, which create holes in the valence band. In n-type
semiconductors, the doping introduces donor impurities, which create electrons in the conduction
band.
By doping the semiconductor material, the Fermi level can be shifted, creating either a resistive-
like connection or a diode-like connection. In a resistive-like connection, the Fermi level is near the
middle of the bandgap, and the current flows in both directions. In a diode-like connection, the
Fermi level is closer to the conduction or valence band, depending on the type of semiconductor
material, and the current flows in only one direction.
The discovery of the Schottky diode and experiments with P-metal and N-metal junctions have
greatly contributed to the development of modern electronics. Schottky diodes have found wide
applications in areas such as power conversion, radio frequency detection, and digital electronics.
The ability to manipulate the Fermi level of semiconductor materials through doping has enabled
the development of advanced semiconductor devices such as transistors, integrated circuits, and
light-emitting diodes.

In a tubular water-filled capacitor, water molecules
are ionized due to the presence of an electric field between the two tubular plates. This ionization
process is important in understanding the behavior of the capacitor, as it can lead to dielectric
breakdown and other issues.
When an electric field is applied to the water-filled capacitor, the water molecules become
polarized, with the positive ends of the molecules orienting towards the negative plate and the
negative ends orienting towards the positive plate. As the electric field increases, the polarization
becomes stronger, and some of the water molecules are ionized, releasing H+ and OH- ions into
the water.
Over-ionization can occur if the electric field becomes too strong, leading to the breakdown of
the dielectric and the formation of a conducting path between the two plates. This can cause a
sudden discharge of the stored energy in the capacitor, leading to damage or failure of the system.
Dielectric breakdown can also occur if the water contains impurities or dissolved ions that can
enhance the conductivity of the water and decrease the dielectric strength.
Ionization of the Water
Molecule

The ionization process in the water-filled capacitor leads to the formation of H+ and OH- ions in the
water. The H+ ions are positively charged and are attracted towards the negative plate, while the
OH- ions are negatively charged and are attracted towards the positive plate. This movement of
ions in the water creates an electric current, which can affect the behavior of the capacitor and
lead to issues such as self-discharge and leakage current.
The creation of H+ and OH- ions in the water-filled capacitor can also have other effects, such as
affecting the pH of the water. As H+ ions are released into the water, the pH of the water becomes
more acidic, while the release of OH- ions can make the water more basic. The pH of the water can
affect the behavior of the capacitor, as changes in pH can alter the conductivity and dielectric
properties of the water.
In conclusion, the ionization of water molecules in a tubular water-filled capacitor is an important
process that can affect the behavior of the capacitor. Over-ionization can lead to dielectric
breakdown, while the creation of H+ and OH- ions can affect the pH and conductivity of the water.
Understanding these processes is important in designing and operating water-filled capacitors for
various applications.

The dielectric constant, also known as
the relative permittivity, is a measure of a material's ability to store electrical energy in an
electric field. In the case of water, the dielectric constant is relatively high, making it an effective
dielectric material for use in electrical circuits.
When water is used as a dielectric material in an electrical circuit, it behaves as a resistor, limiting
the flow of electrical current through the circuit. The resistance of the water depends on several
factors, including the concentration of ions and impurities in the water, the temperature, and the
applied electric field.
The resistance of water as a dielectric material can be modeled using Ohm's Law, which states that
the current flowing through a resistor is directly proportional to the voltage across the resistor and
inversely proportional to the resistance of the resistor. In the case of water, the resistance can be
affected by the dielectric constant, which determines the amount of electrical energy that can be
stored in the water.
The dielectric constant of water is influenced by the presence of ions and molecules in the water,
as well as the temperature and pressure of the water. At room temperature and standard pressure,
the dielectric constant of water is approximately 80, making it an effective dielectric material for
use in electrical circuits.
The dielectric constant of water also influences the capacitance of the circuit, which is a measure
of the amount of electrical charge that can be stored in the circuit for a given voltage. The
capacitance of a circuit containing water as a dielectric material can be calculated using the
equation C = εA/d, where C is the capacitance, ε is the dielectric constant of water, A is the area of
The Dielectric Constant of
Water

the plates in the capacitor, and d is the distance between the plates.
In addition to its use as a dielectric material, water can also act as a capacitor itself, storing
electrical charge in the form of ions and molecules in the water. This can lead to self-discharge and
leakage currents in the circuit, which can affect the performance of the circuit over time.
The relative permittivity, also known as the dielectric constant, of water in a capacitor is an
important property that affects the behavior of the capacitor. The dielectric constant of water
varies with frequency and temperature, and different frequency ranges can have different effects
on the various types of polarizability in water.
Ionic polarizability in water occurs when ions in the water are attracted to the opposite charge
on the plates of the capacitor, causing the water to become polarized. At low frequencies, ionic
polarizability dominates, and the dielectric constant of water increases. This can cause the
capacitance of the capacitor to increase as well, allowing it to store more charge at low
frequencies.
Atomic and vibrational polarizability in water occurs when the electric field of the capacitor
causes the atoms and molecules in the water to vibrate, leading to polarization of the water
molecules. This type of polarizability is most effective at intermediate frequencies, typically
between 1 MHz and 1 GHz. At these frequencies, the dielectric constant of water is high, and the
water can store a significant amount of electrical charge.
Electric polarizability in water occurs when the water molecules become aligned in response to the
electric field of the capacitor. This type of polarizability is most effective at high frequencies,
typically above 10 GHz. At these frequencies, the water molecules become polarized quickly,
allowing the capacitor to store charge rapidly.
Dipolar polarizability in water occurs when the water molecules themselves have an inherent
dipole moment, causing them to become polarized in response to the electric field of the capacitor.
This type of polarizability is most effective at frequencies below 1 MHz, where the dielectric

constant of water is low.
In conclusion, the dielectric constant of water is an important property that influences its
behavior as a resistor in an electrical circuit. Understanding the resistance and capacitance
of water in electrical circuits is important in designing and optimizing the performance of
electrical systems that utilize water as a dielectric material. The relative permittivity of water
in a capacitor depends on the frequency and temperature of the system. Different types of
polarizability in water, such as ionic, atomic/vibrational, electric, and dipolar, are
affected differently by different frequency ranges. Understanding these effects is important
in designing and optimizing the performance of electrical systems that utilize water as a
dielectric material.

Hydrogen bonds are a type of intermolecular force that occurs when a hydrogen atom, covalently
bonded to an electronegative atom, such as oxygen or nitrogen, interacts with a neighboring
electronegative atom in another molecule. Hydrogen bonds are responsible for many important
properties of substances, such as the high boiling point of water and the stability of protein and
DNA structures.
To understand how hydrogen bonds form, it is important to first understand the basic structure of a
water molecule. A water molecule consists of two hydrogen atoms covalently bonded to a single
oxygen atom. Due to the electronegativity of the oxygen atom, the electrons in the covalent bonds
are more attracted to the oxygen atom, creating a partial negative charge on the oxygen and a
partial positive charge on the hydrogen atoms.
When two water molecules come close together, the partial positive charge of one hydrogen atom
is attracted to the partial negative charge of the oxygen atom in the other molecule, forming a
hydrogen bond. This interaction is not as strong as a covalent bond, but it is strong enough to
cause water molecules to stick together, which is why water has a high surface tension and can
form droplets.
Hydrogen bonds are also responsible for the unique properties of water, such as its high boiling
point and heat capacity. When heat is added to water, the energy is used to break the hydrogen
bonds between water molecules, rather than increasing the kinetic energy of the molecules. This
means that water can absorb a lot of heat energy without changing temperature, making it an
effective coolant.
Hydrogen Bonds

Microwaves, on the other hand, heat water through a different mechanism. Microwaves are a form
of electromagnetic radiation that can be absorbed by water molecules, causing them to vibrate
rapidly and generate heat. This is why microwaves are effective at heating water-based
substances, such as food or beverages.
In summary, hydrogen bonds are a type of intermolecular force that occurs when a hydrogen
atom interacts with an electronegative atom in another molecule. They are responsible for
many important properties of substances, such as the high boiling point of water and the
stability of protein and DNA structures. Microwaves, on the other hand, heat water through
the absorption of electromagnetic radiation, causing water molecules to vibrate and
generate heat.

Electrical pulse period manipulation
and polarization in a water capacitor is a fascinating area of study that has the potential to
revolutionize the field of energy storage. In this article, we will explore the concepts of pulse period
manipulation and polarization in water capacitors, their significance, and the current state of
research in this field.
A capacitor is a device that stores electric charge. It consists of two conducting plates separated by
an insulating material, also known as a dielectric. The capacitance of a capacitor depends on the
surface area of the plates, the distance between them, and the properties of the dielectric. A water
capacitor is a type of capacitor where the dielectric is water.
One of the interesting properties of water is that it can be polarized by an electric field. This means
that when an electric field is applied to water, the water molecules align themselves with the field,
creating a dipole moment. The degree of polarization depends on the strength of the electric field
and the properties of the water.
Pulse period manipulation is a technique where electrical pulses are applied to a water capacitor at
specific time intervals. The pulse period refers to the time interval between the application of
successive pulses. By manipulating the pulse period, researchers can control the polarization of the
water in the capacitor.
Recent research has shown that pulse period manipulation can significantly increase the energy
density of water capacitors. Energy density is a measure of the amount of energy stored per unit
volume or mass. By controlling the polarization of the water, researchers can increase the energy
Pulse Period Manipulation
and Polarization

density of the capacitor, making it a more efficient energy storage device.
In addition to pulse period manipulation, researchers are also studying the effects of electrode
materials on the polarization of water capacitors. The choice of electrode material can have a
significant impact on the performance of the capacitor. For example, research has shown that
using carbon-based electrodes can enhance the polarization of water, leading to higher energy
densities.
Water capacitors have several advantages over traditional energy storage devices, such as
batteries. They are non-toxic, non-flammable, and have a longer lifespan. In addition, they can
store large amounts of energy and can be charged and discharged quickly.

electrical-polarization-process.pdf

If you're looking to orient water molecules in an electric field, a relatively modest electric field can
achieve this because water is a polar molecule. To align a water molecule, an electric field on the
order of 1 kV/cm is often more than enough. Given a 1/8" gap (approximately 0.318 cm), this would
equate to a voltage of approximately 318 volts.
In its neutral state, a hydrogen atom is not electropositive. The hydrogen atom consists of one
proton and one electron, and it is electrically neutral because the positive charge of the proton
balances the negative charge of the electron. However, hydrogen can become a positive ion (a
proton) if it loses its electron, such as through ionization.
If you're dealing with ionized hydrogen (protons), these would indeed be repelled by a positive
electric field and attracted to a negative one. If the hydrogen atoms are not ionized, they would not
be significantly affected by an electric field because they are overall electrically neutral.
If you're trying to manipulate neutral hydrogen atoms with an electric field, you may need to ionize
them first. Ionization typically requires a significant amount of energy and can be achieved in
various ways, such as with a high voltage, intense light, or high temperatures.
The process of converting a neutral hydrogen atom into a positively charged ion (a proton, H+) is
called ionization. For hydrogen, this involves removing the single electron from the atom. There are
several methods that can be used to achieve this:
1. Electrical Discharge: Passing a high-voltage electric current through the gas can strip
electrons from their parent atoms, creating ions. This is the principle behind techniques
like glow discharge and arc discharge.
2. Electron Impact: High-energy electrons can knock electrons off atoms to create ions.
This often happens in devices like mass spectrometers.
3. Photoionization: High-energy photons (such as ultraviolet light or X-rays) can also ionize
atoms by knocking off electrons.
4. Thermal Ionization: At very high temperatures, the kinetic energy of the atoms can be
high enough to cause ionization. This is what happens in the sun and other stars.
5. Chemical Ionization: Certain chemical reactions can result in ionization. For example,
some strong acids can ionize hydrogen.
Molecule & Gas Atom
Ionization - Raising H+ to
13.6 electronVolts

Sure, let's delve deeper into these three methods:
1. Electrical Discharge Ionization: This is the process of ionizing a gas by applying a high
voltage between two electrodes. When the voltage is sufficiently high, it can accelerate
free electrons, which then collide with neutral gas atoms. If the kinetic energy of the
electron is high enough, it can knock an electron off the atom, creating an ion. This
process can create a plasma, a gas of ions and free electrons.
Glow discharge and arc discharge are two forms of electrical discharge. Glow discharge
operates at lower pressures and voltages, while arc discharge operates at higher
pressures and voltages.
In your context, you could potentially use an electrical discharge to ionize your hydrogen
gas. You would need to carefully contain and control the discharge to ensure safety, as
the process can produce heat and UV light.
2. Electron Impact Ionization (also known as Collision Ionization): This method is
similar to electrical discharge but is usually discussed in the context of a beam of high-
energy electrons colliding with a gas. When a high-energy electron collides with a neutral
atom, it can knock off one of the atom's electrons, creating an ion.
This method is often used in instruments like mass spectrometers to ionize samples. It's
typically used in vacuum conditions, as the mean free path of the electrons needs to be
long enough for them to gain sufficient energy before they collide with the atoms.
3. Photoionization: This is the process of ionizing an atom using photons, which are
particles of light. When a photon with enough energy collides with an atom, it can knock
an electron off the atom, creating an ion. The minimum energy required to ionize the
atom is called the ionization energy.
For hydrogen, the ionization energy is 13.6 electron volts (eV), which corresponds to
ultraviolet light with a wavelength of about 91.2 nm. So you would need light of this
energy or higher to photoionize hydrogen.
Photoionization can be a very clean method of ionization, as it doesn't introduce any new
particles into the system. However, producing light of the required energy can be
challenging. UV lasers can do this, but they tend to be expensive and require careful
handling due to the hazards of UV light.
Again, all of these methods involve significant energy and can be hazardous if not handled
correctly. Always follow appropriate safety procedures, and consider consulting with an expert if
you're unsure.
ChatGP
The electronvolt (eV) is a unit of energy that is often used in the context of atoms and subatomic
particles, like electrons. One electronvolt is defined as the amount of kinetic energy gained (or lost)
by a single electron accelerating from rest through an electric potential difference of one volt.

So, when we say that the ionization energy of hydrogen is about 13.6 eV, it means that it takes
13.6 eV of energy to remove an electron from a hydrogen atom (in its ground state).
This energy isn't directly related to the input voltage of a circuit or device. The input voltage can
create an electric field, and this field can accelerate charged particles. If a charged particle (like an
electron) accelerates through a voltage difference of one volt, it will gain (or lose) an energy of one
electronvolt.
But to use voltage to ionize an atom, you need a situation where free electrons can be accelerated
by the electric field to gain enough kinetic energy. This can happen in an electrical discharge, for
example, where a high voltage can ionize a gas. The voltage needed to achieve this can be much
higher than the ionization energy of the atoms (in eV), due to inefficiencies and losses in the
process. The specific voltage needed can depend on many factors, such as the pressure and
composition of the gas, the distance between the electrodes, and the design of the device.
As always, dealing with high voltages and ionization processes can involve significant hazards, and
it's important to follow all relevant safety procedures and guidelines.
The water capacitor is 2 - 3" tubes, 1/2" inner and 3/4" outer SS304L. the gap is approx
1/8". what do the electric field voltage requirements look like for this?
The electric field strength (E) in a capacitor is given by the formula E = V/d, where V is the voltage
across the capacitor and d is the distance between the plates (or in this case, tubes). The electric
field is usually measured in volts per meter (V/m).
The 1/8" gap between your tubes is about 0.003175 meters. If you were to apply a voltage of 1 volt
across the tubes, the electric field strength would be E = 1V / 0.003175m = 315 V/m.
If you're looking to ionize hydrogen, as discussed earlier, you'd need an electric field that's strong
enough to give electrons enough energy to escape their atoms. This would likely require a field on
the order of kilovolts per millimeter or higher. For a 1/8" (about 3.175mm) gap, this could mean a
voltage of several kilovolts.
However, creating such a strong electric field in a gas at atmospheric pressure would likely lead to
electrical breakdown and a spark or arc, rather than ionization of individual atoms. To achieve
controlled ionization, you would typically need a vacuum or very low pressure, so the mean free
path of the electrons is long enough for them to gain sufficient energy before they collide with
another atom.
If you're simply looking to align water molecules with an electric field, you would not need such a
high field strength. A field of a few kV/m (equivalent to a few volts across the tubes) could be
sufficient.
In any case, working with high voltages can be dangerous, and it's important to take all necessary
safety precautions. Consider consulting with an expert or professional if you're unsure.
what field strength is needed to apply the 13.6eV

ChatGP
In order to understand how much field strength is required to apply the 13.6 electronvolt (eV)
needed to ionize a hydrogen atom, we need to take into account the concept of work done.
The work done (W) on a particle by an electric field as it moves through a distance (d) is given by
W = qEd, where q is the charge of the particle and E is the electric field strength. If we want to give
an electron an energy of 13.6 eV, we can set W equal to this value.
The charge of an electron (q) is about 1.6 x 10^-19 Coulombs. So, if we want to give an electron an
energy of 13.6 eV (which is about 2.18 x 10^-18 Joules), we can rearrange the equation to solve for
E:
E = W / (q*d) = (2.18 x 10^-18 J) / [(1.6 x 10^-19 C) * d]
For a 1/8" (about 0.003175 m) gap, this gives:
E = (2.18 x 10^-18 J) / [(1.6 x 10^-19 C) * 0.003175 m] ≈ 4.3 x 10^7 V/m
This means that you would need an electric field of about 43 million volts per meter to give an
electron an energy of 13.6 eV over a distance of 1/8". That corresponds to a voltage of
approximately 136.5 kV across the 1/8" gap.
However, these calculations are a simplification, and they assume that the electron is free to move
across the entire gap without any collisions. In reality, the mean free path of an electron (the
average distance it can travel before colliding with an atom) in air at atmospheric pressure is much
less than 1/8", and so the electron would not be able to gain this much energy before it collided
with an atom.
Therefore, to achieve ionization in a controlled manner, you would typically need a vacuum or very
low pressure, and the voltage required would depend on the specific conditions.
As always, working with high voltages can be dangerous, and it's important to follow all necessary
safety precautions. Consult with an expert or professional if you're unsure.
ok how about a 1/16" gap
ChatG
With a reduced gap distance of 1/16" or approximately 0.0015875 meters, we use the same
formula for the electric field:
E = W / (q*d)

To calculate the required voltage (V), we remember that electric field strength (E) is voltage (V)
divided by distance (d). So we can rearrange the formula to find V = E*d:
V = E*d = W / q
Using the numbers we established before (W = 2.18 x 10^-18 J and q = 1.6 x 10^-19 C), we find:
V = (2.18 x 10^-18 J) / (1.6 x 10^-19 C) ≈ 13.625 kV
So the voltage required across the 1/16" gap to provide an electron with 13.6 eV of energy would
be approximately 13.625 kV.
Again, in reality, achieving ionization under atmospheric pressure conditions would likely require
higher voltages due to factors like electron collision and energy loss. Always take proper
precautions when dealing with high voltage systems.
Te result is a magnitude of 10
1/16" = 13.6kV = 13.6eV
1/8" = 136.5kV = 13.6eV

GPT Interpretation from: https://stanslegacy.com/books/us-patents/page/gas-generator-
voltage-control-circuit-4798661
L-1. Voltage and Current Regulation: The use of a uni-polar pulsating DC voltage is an initial
approach to raise the amplitude of the voltage without electron leakage. However, it has a limit up
to an amplitude of 4.0 volts. This is represented by level L-1 in Fig. 8.
L-2. Duty Cycle Variation: To further restrict current flow with amplitude voltages above L-1, the
duty cycle pulse of the pulsed DC voltages can be varied (as shown in FIGS. 2, 3, and 8). This can
help control and limit the electron leakage from the exciter plate which has negative voltage
applied. The voltage amplitude limit in this approach is 4.0 volts, as represented by L-2 in Fig. 8.
L-3. Pulsed DC Voltage: The pulsing of the pulsed DC voltage, which comprises switching the
voltage on and off periodically, can help in the function of inhibiting electron leakage. The duty
pulses have an effective amplitude in inhibiting electron leakage by controlling the force on the
electrons around the plate exciter, having the negative potential voltage applied. The amplitude is
effective to increase the output gas generation with an upper limit of 5.5 volts, in this instance L-3
of Fig. 8.
L-4. Serially Connected Exciter Plates: Though serially connected exciter plates do permit a
higher amplitude of voltage to be applied, it too, has a limitation L-4 of 7 volts. This method allows
the positive voltage to be applied individually to each of the outer plate exciters and the negative
voltage to each of the inner plate exciters, which increases the surface between the inner and
outer plates, thus reducing the probability of an electron breaking free and leaking to the attractive
field of the positive voltage plate.
L-5. Use of Resistors as Current Inhibitors: Resistors, such as resistor 60 shown in FIGS. 1 and
5, can act as simple current inhibitors to prevent electron leakage. These resistors can be fine-
tuned for specific applications and are connected to each of the plates having the negative voltage
connected thereto. They effectively raise the voltage amplitude limit to 8.5 volts before breakdown,
as shown at L-5 in Fig. 8.
Beyond L-5. Use of Poor Conductive Material: Using a material that is a poor conductor of
electricity, like stainless steel 304L, can further inhibit electron leakage. This material is used in the
electron inhibitor, shown in FIG. 7, which is connected between the inner plate (having the negative
potential connected to it) and ground. Stainless steel 304L is considered a poor conductor when
compared to materials like copper or gold, and can effectively restrict the electron flow, thus
Voltage Threshold & Amp
Restriction Levels

reducing electron leakage. This technique removes the upper level of amplitude of the voltage as
shown beyond L-5 in Fig. 8. Fine-tuning of the resistive value of the electron inhibitor is achieved
by changing the resistive material to binder ratio, and by the use of resistor 75 connected in series.
The varying of the duty cycle of the uni-polar DC voltage pulses is a technique used to control the
amplitude of the voltage and thereby inhibit electron leakage. This variation can be periodic or
aperiodic:
Periodic Variation of Amplitude (Claim 7):
In the periodic variation of amplitude, the on/off pattern of the duty cycle of the uni-polar DC
voltage pulses repeats at regular intervals. This could involve, for example, turning on the voltage
for one second, then turning it off for one second, and repeating this pattern continuously. This
form of periodic variation can help maintain a certain average voltage amplitude, preventing
electron leakage by keeping the voltage within safe limits.
Aperiodic Variation of Amplitude (Claim 8):
On the other hand, in the aperiodic variation of amplitude, the duty cycle of the uni-polar DC
voltage pulses changes irregularly or randomly. For instance, the voltage might be on for two
seconds, then off for one second, then on for half a second, and so forth, with no consistent
pattern. This form of aperiodic variation might be useful in systems where the conditions fluctuate
or where a certain level of randomness is beneficial. As in the case of periodic variation, the aim is
to maintain an average voltage amplitude that minimizes electron leakage.

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