USPatent applicationPatented

Staged emitter-attractor ion drive

Granted 17 Apr 2007 · 1 office action

Current assignee: Aerojet Rocketdyne, Inc. · originally RTX Corporation

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Inventors: Benjamin Goldberg, Alan B. Minick · Examiner: L. J. Casaregola · AU 3746 · TC 3700

Life of the application

15 dated events
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Abstract

An ion drive system for creating a propulsion force or thrust has at least one stage having an emitter and an attractor spaced from the emitter by a gap. An ionizable dielectric media is located within the gap. The drive system further has a propellant source for introducing a propellant in the vicinity of the emitter and a power source for creating a high intensity field in the vicinity of the emitter to ionize the dielectric media and a diffused field in the vicinity of the attractor to accelerate the ions away from the emitter and thereby create a propulsive force. In a preferred embodiment, the ion drive system has a plurality of stages.

Description

4 parts
›BACKGROUND OF THE INVENTION

(1) Field of the Invention

The present invention is directed to a drive system for creating a propulsive force and in particular to a staged emitter-attractor ion drive system.

(2) Prior Art

Many different propulsion systems are known in the prior art. For example, there are systems for generating a thrust force using propellants and rocket motors. There are other systems involving the use of jet engines.

Despite the existence of a wide variety of propulsions systems, there remains a need for advanced drive systems. Particularly for supplying a propulsion force to a spacecraft.

›SUMMARY OF THE INVENTION

Accordingly, it is an object of the present invention to provide an improved ion drive system for generating a propulsive force.

It is a further object of the present invention to provide a drive system which may be used to propel spacecraft and other vehicles.

The foregoing objects are attained by the present invention.

In accordance with the present invention, an ion drive system broadly comprises at least one stage having an emitter and an attractor spaced from the emitter by a gap. An ionizable dielectric media is located within the gap. The drive system further has a propellant source for introducing a propellant in the vicinity of the emitter and a power source for creating a high intensity field in the vicinity of the emitter to ionize the dielectric media and a diffused field in the vicinity of the attractor to accelerate the ions away from the emitter and thereby create a propulsive force. In a preferred embodiment, the ion drive system has a plurality of stages.

Other details of the staged emitter-attractor ion drive of the present invention, as well as other objects and advantages attendant thereto, are set forth in the following detailed description and the accompanying drawings, wherein like reference numerals depict like elements.

›BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic representation of an one stage ion drive system;

FIG. 2 is a schematic representation showing the ion and force characteristics of the drive system of FIG. 1 ; and

FIG. 3 is a schematic representation of a staged emitter-attractor ion drive system in accordance with the present invention.

›DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT(S)

The use of intense electric fields to create ions has been used in many applications. Repulsion of like charges after ionization has been used to accelerate ions away from an ionization source. The present invention recognizes this as a possible propulsion source. The present invention makes use of a combination of concentrated and distributed fields to repeatedly accelerate the initial ions, increasing their propulsive benefits without requiring an increase in a propellant flow.

Referring now to FIG. 1 , one stage of an ion drive system comprises an emitter 10 and an attractor (receiver) 12 spaced from the emitter 10 . The emitter 10 and the attractor 12 may be made from any suitable electrically conductive material known in the art. For example, the emitter 10 and/or the attractor 12 may be formed from a carbon fiber material or from nanotubes. The emitter 10 is an ionization feature so it is much smaller in area than the attractor 12 . In fact, the smaller and the sharper the emitter 10 is, the better. If desired, alpha particle emitters, such as americium, can be used to further enhance the ionization. The emitter 10 and the attractor 12 are electrically connected to a high voltage source 14 . The high voltage source 14 may be a DC source or a pulsating direct current (PDC) source.

The ion drive system includes a propellant source 16 for discharging a propellant towards the emitter 10 . The propellant may comprise any suitable propellant known in the art such as any stable gas including, but not limited to, the atmosphere. The propellant must be largely nonconductive, so water will not work. In operation, the propellant is ionized and not detonated.

One of the unique aspects of the ion drive system of the present invention is that it does not require any chamber or discharge nozzle. One of the special features of the ion drive system of the present invention is that it can be applied conformally to any body or wing and apply the propulsion over any surface, while reducing the boundary layer and reattaching the flow.

In each stage, a high intensity electric field, approaching the fluid breakdown potential, is preferably generated on the emitter 10 , which has a reduced surface area as compared to the surface area of the attractor 12 , when the emitter 10 is placed in the vicinity of the increased surface area attractor 12 . The field concentration varies with a primary proportionality based on the ratio of the emitter surface area to the attractor surface area, concentrating the intense field around the emitter 10 while creating a diffused field around the attractor 12 . The emitter-attractor gap distance D and the dielectric of the media in the gap further tailor the field intensities. The gap distance D may vary from approximately 0.001 inches to 6.0 inches. Further tailoring of the field can be accomplished through tailored or stratified dielectric modifications in the emitter-receiver gap, and through positioning of adjacent diffused fields. By putting coatings on the emitter, or attractor, or between them, the field shape and local intensity can be changed. By putting charged plates of lower intensity near the device, one can focus the field and flow by distorting the drive field.

As an ionizable dielectric media such as lithium, argon, xenon, etc. may be introduced at the high intensity field, ionization occurs. Preferably, the ionizable dielectric media has a low ionization potential. As shown in FIG. 2 , the created ion bears the same charge as the ionizing source (the emitter 10 ) and is repelled. The present invention utilizes the attractor 12 with a diffused field insufficient to initiate ionization but strong enough to attract the ions being repelled by the ionization source. This attraction both continues to accelerate the ions and accelerates the attractor 12 towards the created ions. Both actions add to the forward propulsion. As the ion passes through the diffused attractor/receiver 12 , field deionization may occur. Regardless, most ions pass adjacent to the receiver 12 while maintaining momentum away from the emitter 10 . The foregoing describes a single stage emitter-attractor staged ion drive system for creating a propulsive force.

Referring now to FIG. 3 , an ion drive system 20 is shown in which additional stages have been added. The stages each contain an emitter 10 and an attractor 12 . As can be seen, each of the emitters 10 and the attractors 12 are electrically connected to a common power source 14 . In this type of system, the additional stages must be isolated to prevent reverse flow of oppositely charged particles, reducing propulsion effectiveness. Two measures may be used to accomplish this isolation. The first is to reverse the polarity of adjacent emitter-receiver pairs. This is demonstrated in FIG. 3 . The second is to position the subsequent emitter 10 downstream of the prior stage diffused receiver field. Since these are similarly polarized, reverse flow is prevented while augmenting the attractive field strength of the prior attractor/receiver 12 .

The ion drive systems of the present invention have particular utility for space vehicle propulsion systems. For example, they can be used to achieve orbital propulsion and for deep space propulsion. Still further, the ion drive systems of the present invention may be used and operated in the atmosphere and in a vacuum. The ion drive systems may also be used for high altitude propulsion, silent propulsion, and thrust augmentation on other types of vehicles.

It is apparent that there has been provided in accordance with the present invention a staged emitter-attractor ion drive which fully satisfies the objects, means, and advantages set forth hereinbefore. While the present invention has been described in the context of specific embodiments thereof, other alternatives, modifications, and variations will become apparent to those skilled in the art having read the foregoing description. Accordingly, it is intended to embrace those alternatives, modifications, and variations which fall within the broad scope of the appended claims.

Claims as granted

14 claims

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Classifications

3 codes
IPC · International Patent Classification
Section F — Mechanical engineering; lighting; heating; weapons
  • F03H1/00
USPC · US Patent Classification
60/20260/204

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File wrapper

⤢ drag to zoomJul 2004Oct 2004Jan 2005Apr 2005Jul 2005Oct 2005Jan 2006Apr 2006Jul 2006Oct 2006Jan 2007Apr 2007USPTOApplicantNon-final rejectionResponse after non-final
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Pendency
2.7 y
1,000 days filing → grant
Office actions
1
non-final + final
Responses
1
no RCE
Examiner
L. J. Casaregola
art unit 3746 · TC 3700
Citations: 3 back · 1 forward

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Chain of title

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