Lockheed Martin Corporation v. Space Systems/loral, Inc.

249 F.3d 1314, 58 U.S.P.Q. 2d (BNA) 1671, 2001 U.S. App. LEXIS 7894, 2001 WL 436028
CourtCourt of Appeals for the Federal Circuit
DecidedApril 30, 2001
Docket00-1310
StatusPublished
Cited by30 cases

This text of 249 F.3d 1314 (Lockheed Martin Corporation v. Space Systems/loral, Inc.) is published on Counsel Stack Legal Research, covering Court of Appeals for the Federal Circuit primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Lockheed Martin Corporation v. Space Systems/loral, Inc., 249 F.3d 1314, 58 U.S.P.Q. 2d (BNA) 1671, 2001 U.S. App. LEXIS 7894, 2001 WL 436028 (Fed. Cir. 2001).

Opinion

DECISION

GAJARSA, Circuit Judge.

Lockheed Martin Corporation (“Lockheed”) is the assignee of United States Patent 4,084,772 (“the '772 Patent”), which discloses an apparatus and method for steering a satellite. In 1995, Lockheed’s predecessor, Martin Marietta Corporation, brought this patent infringement action against Space Systems/Loral, Inc. (“SSL”), alleging that certain SSL satellites infringe the '772 Patent. On March 7, 2000, the United States District Court for the Northern District of California (“District Court”) determined that certain limitations required by claim 1 of the '772 Patent are not present in SSL’s Intelsat VII satellites either literally or under the doctrine of equivalents, and granted SSL’s motion for summary judgment. Lockheed Martin Corp. v. Space Systems/Loral, 88 F.Supp.2d 1095, 1102 (N.D.Cal.2000). Lockheed appeals that judgment.

For the reasons discussed below, we affirm.

I. BACKGROUND

The '772 Patent, entitled “Roll/Yaw Body Steering for Momentum Biased Spacecraft,” claims a structure and method for reducing the pointing errors of a satellite that has entered into an inclined orbit by varying the speed of the satellite’s transverse momentum wheel in a sinusoidal manner.

A. Introduction

A communications satellite typically orbits the earth in a geosynchronous equatorial orbit, circling the earth once every twenty-four hours in the equatorial plane. A geosynchronous orbit in the equatorial plane allows a satellite to maintain the same position relative to fixed points on the earth’s surface, and is often referred to as “geostationary.” A satellite in geostationary orbit, when viewed from the ground, appears to remain stationary in the sky. Therefore, a geostationary orbit enables a communications satellite to maintain a constant relationship with transmitters on earth. In addition to preserving a geosynchronous equatorial orbit, a communications satellite must also maintain a proper “attitude,” or pointing direction, so that its antennae remain pointed at the desired target on the earth.

While in orbit, however, a satellite is subject to various destabilizing forces such as the gravitational effects of the sun and the moon. Such forces may cause a satellite to drift out of its equatorial orbit, into an “inclined” north-south orbit. A satellite in an inclined orbit may still orbit the earth in a geosynchronous manner (once every twenty-four hours), but may no longer appear stationary in the sky to an earthbound observer. The following diagram, Figure 2 of the '772 Patent specification, depicts an inclined orbit relative to an equatorial orbit:

*1317 [[Image here]]

Therefore, in an inclined orbit, the antennae of a communications satellite point north of the equator for half of the orbit and south of the equator for half of the orbit. Unless the satellite corrects for solar and lunar gravitational effects, the orbit of a geosynchronous satellite acquires an inclination at the rate of about 0.8 degrees annually.

The '772 Patent discloses a system for allowing a communications satellite to continue to operate effectively after entering an inclined orbit. It does so by changing the attitude, or pointing direction, of the satellite when the satellite is north and south of the equator. The method described by the '772 Patent rotates the satellite so that its antennae point north or south, and remain pointed at the same earth target over the course of twenty-four hours.

The attitude of satellites is described in terms of movement and rotation about three axes. The “pitch” axis lies in a north-south direction, the “roll” axis points in the direction of satellite orbital movement, and the “yaw” axis points to the center of the earth. In an inclined orbit, roll pointing error occurs when a satellite is north or south of the equator. There is no roll pointing error when a satellite crosses the equator twice each orbit (depicted above in diagram 2 at points B and D). Conversely, yaw pointing error is greatest when a satellite crosses the equator. There is no yaw pointing error when a satellite is furthest north or south of the equator (depicted above in diagram 2 at points A and C).

The structure and method described by the '772 Patent rotates a satellite around its roll axis such that its antennae point to the south when the satellite is north of the equator, and point to the north when the satellite is south of the equator. In this manner, even though a satellite is moving north and south during its orbit, it remains pointed at the same earth target, and behaves as if it were still in geostationary orbit.

B. The '772 Patent Technology

Many communication satellites employ at least one “momentum” or “reaction” wheel centered on the pitch axis of a satellite (“pitch wheel”) powered by an electric motor. A spinning momentum wheel creates angular momentum, or “stiffness,” and opposes any satellite rotation about *1318 the roll or yaw axis. In other words, the spinning pitch wheel acts like a gyroscope, resists external forces, and keeps the pitch axis pointed in a north-south direction.

In addition to this resistance effect, momentum wheels also cause a satellite to rotate around its axes by taking advantage of the physical law of conservation of angular momentum. When a momentum wheel increases speed in one direction, it causes the entire satellite to spin in the opposite direction along the same axis in order to conserve angular momentum. Thus, through careful control of momentum wheels centered on different axes, a proper satellite attitude can be maintained.

As discussed above, the invention described by the '772 Patent is a structure and method for spinning a second momentum wheel centered on a satellite’s yaw axis. This wheel is referred to as the “yaw” wheel or “transverse” wheel. When the yaw wheel is accelerated, it creates angular momentum about the yaw axis. In response, the pitch wheel and the entire satellite must rotate about the roll axis in order to compensate and cancel the angular momentum created by the yaw wheel, thereby adjusting the north-south pointing direction of the antennae.

As described by the '772 Patent, the amount of north-south roll pointing attitude adjustment varies with the speed and spin direction of the yaw wheel. When the yaw wheel is not spinning, the satellite does not rotate about its roll axis. However, increased yaw wheel speed in one direction points the satellite to the north; increased yaw wheel speed in the other direction points the satellite to the south. In short, by varying the speed and direction of the yaw wheel, the satellite can be steered about its roll axis, adjusting and correcting for the north-south roll pointing errors described above.

The following diagram, Figure 3 of the '772 Patent specification, depicts the pointing direction resulting from this roll pointing attitude adjustment. As depicted, by rotating the satellite around its roll axis by Ó degrees, the satellite points at the equator:

[[Image here]]

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249 F.3d 1314, 58 U.S.P.Q. 2d (BNA) 1671, 2001 U.S. App. LEXIS 7894, 2001 WL 436028, Counsel Stack Legal Research, https://law.counselstack.com/opinion/lockheed-martin-corporation-v-space-systemsloral-inc-cafc-2001.