Gas Atom

ionized ambient air gases (104)

To obtain higher energy-yields beyond the normal gas combustion process, ionized ambient air gases (104) of Figure (3-31) is, now, exposed to and intermixed with Fuel-Gases (88) prior to thermal gas ignition (98) of Figure (3-38), as illustrated in (240) of Figure (3-31).

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ionized gases (104)

As ambient air gases (101) enters into and passes through air filter chamber (105) toward and beyond air gate assembly (GG), the moving air gases (101) are exposed to high energy voltage fields (up to and beyond 2,000 volts) (106/107) of opposite electrical polarity which causes ambient air gases to become ionized gases (104), as illustrated in (260) of Figure (3-33).

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Once electron ejection occurs, the liberated and free floating electrons (117a xxx 117n) continue to migrate toward positive voltage zone (106); whereas, the newly formed ionized gas atom (having missing electrons) (104) continues to move onward and through air intake manifold (109) of Figure (3-31) to engine cylinder (102) of Figure (3-38).

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ionized gas vapor (104a xxx 104n)

The newly established and on-going electron conversion process (390) continues to aid ionized gas process (260) as other gas atoms (101a xxx 101n) are destabilized into ionized gas vapor (104a xxx 104n).

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gas atom (104)

To further destabilize gas atom (104), emitted laser energy (electromagnetic energy having zero mass) (116) is, now, injected into Gas Resonant Cavity (410) via optical lens (121) and superimposed onto gas ionized process (260) and subsequently absorbed by gas atom nucleus (108), as illustrated in (260) of Figure (3-33) as to (270) of Figure (3-34).

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... allowing even a greater number of electrons (117a xxx) to be ejected from ionized gas atom (104) being simultaneously subjected to Electron Extraction Process (260), as illustrated in (280) of Figure (3-35).

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ionized gas (104)

… embly (420) of Figure (3-43) is electrically pulsed (126a xxx 126n) via variable pulsing circuit (125) in such a way as to vary light intensity (116) to match the light absorption rate of ionized gas (104), and, is determined with respect to the forward current through Led's (118) by (Eq 15)

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gas atom (104)

Applied voltage amplitude (Va xxx Vn), applied voltage pulse frequency (65a xxx 65n), and applied current pulse train (126a xxx 126n) are design variable to "tune-in" to the resonant properties of gas atom (101) while stimulating and performing gas process (260) which attenuates electrical force (AA') of Figure (3-35) to disrupt the mass equilibrium of gas atom (104).

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sub-critical gas atoms (104a xxx 104n)

The resultant and newly formed sub-critical gas atoms (104a xxx 104n) are directed onward through air intake manifold (109) of Figure (3-31) to and beyond both exhaust gas metering port (370) and injector port (36) where metered fuel-gas (88), metered exhaust gases (99 …

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metered sub-critical gas atoms (104a xxx 104n)

… e manifold (109) of Figure (3-31) to and beyond both exhaust gas metering port (370) and injector port (36) where metered fuel-gas (88), metered exhaust gases (99), and metered sub-critical gas atoms (104a xxx 104n) forms gas-mixture (103) entering engine cylinder (102), as illustrated in (240) of Figure (3-31) as to (340) of Figure (3-38).

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sub-critical gas ions (104a xxx 104n)

Thermal atomic interaction (127) is caused when sub-critical gas ions (104a xxx 104n) (derived from both water bath ~ and ambient air gases) fails to unite with or covalently link up or covalent bond with highly energized (laser primed) hydrogen atom (128).

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