1. Field of the Invention
The present invention relates to systems and devices for stabilizing boats and small ships. More particularly, the present invention relates to gyroscopic stabilizers positioned in boats and configured to counteract rolling motion caused by waves and ship wakes. The gyroscopic stabilizer of the present invention is an active stabilization device.
2. Description of the Prior Art
A rolling boat is uncomfortable and can cause people and animals to experience motion sickness. A device that can create an anti-roll torque can be used to oppose this motion. The difficulty with creating such a device is that a boat is not resting on or in a solid medium that can be used as a base to create an anti-rolling moment. One solution to this problem is to use a large gyroscope to stabilize the boat. A gyroscope is a rotor spinning at a high speed around its spin axis, mounted in a frame that can be moved as the user wishes. When the spinning wheel is turned around an axis (gimbal axis) that is at right angles to its spin axis, a torque is generated around a third axis that is perpendicular to both the spin axis and the turning axis. A gyrostabilizer creates a torque or moment that reduces rolling motion. The gyrostabilizer has a rotor whose spin axis is nominally vertical. The rotor frame is mounted on gimbals so that the rotor can rotate about a transverse, side-to-side axis, but the frame is fastened to the vessel so that the system is constrained to roll from side to side with the boat. With proper selection of the spin and gimbal axes, a torque can be created to oppose roll motion.
Gyroscopic stabilizers (gyrostabilizers) were first used to stabilize very large ships and yachts almost a century ago, and their ability to resist rolling motion (side to side rotation) is well understood. In 1913, the Sperry Gyroscope Company installed a 5-ton gyrostabilizer on the USS Worden, a 700-ton destroyer. Although the device performed as expected, the Navy stopped installing gyrostabilizers at the onset of WW I. Some gyrostabilizers were installed on private yachts in the first part of the 20th century, but other methods of stabilization supplanted gyrostabilizers in the yacht market.
The heart of a gyrostabilizer is a rotor spinning at high speeds. The rotor has three important characteristics:
Weight. The rotor is the heaviest component in the gyrostabilizer machine.
Angular Momentum. The angular (spinning) momentum of the rotor determines its ability to stabilize a yacht or small craft
Kinetic Energy. The kinetic energy stored in the spinning rotor determines how long it takes to start and stop the machine.
The moment of inertia of the rotor depends on both its mass and its mass distribution. The farther mass is located from the spin axis, the higher the moment of inertia that results from the mass. The more the mass of rotor is distributed toward the outer rim of the wheel, the higher the ratio of moment of inertia to its mass.
The angular momentum of the rotor is the rotor's moment of inertia multiplied by its angular speed, and a rotor with high angular momentum can create a large anti-rolling torque. To create a lightweight rotor with a high angular momentum, the designer has to rotate it at high speeds.
The kinetic energy of a spinning rotor is proportional to its moment of inertia and to the square of its speed. The time required to start or stop the rotor is roughly proportional to its full-speed energy, or to the square of its rotation rate.
When a gyroscope is turned around an axis, called the gimbal axis, which is approximately at right angles to its spin axis, it creates a torque around a third axis, orthogonal to the first two. To create an anti-rolling gyrostabilizer, the spin axis is nominally vertical, and the spinning rotor is tipped forward or backwards on a gimbal axis in the boat. The result is a torque orthogonal to both the spin axis and the gimbal axis. Nominally this torque is aligned with the boat's roll axis, and therefore can be utilized as an anti-rolling torque. The strength of this torque depends on the angle formed by the spin axis and the gimbal axis. Assuming that the boat rotation is primarily around its roll axis, and that rotation around the boat's pitch axis is small enough to be ignored, as the tip angle increases, the included angle decreases and the anti-rolling torque decreases. Accordingly, the maximum anti-rolling restoring torque will be limited to the based on maximum gimbal angles of plus or minus ninety-degrees.
Summarizing the tradeoffs described above:
A high-speed rotor can be lighter than a low-speed rotor.
Low speed rotors can startup and shutdown using less power than high-speed rotors.
The minimum moment of inertia of the rotor is determined by the maximum anti-roll torque required by the boat. This is determined by the size of the boat and the size of the waves or wakes.
Apart from the very large scale passive gyrostabilizer developed by Sperry for Navy vessels of World War I, systems designed to stabilize vessels usually rely upon actuated appendages, such as fins, interceptors or submerged foils, to counteract the rolling effects caused by waves and wakes. Fins, interceptors, and foils all depend on significant forward motion for their anti-roll forces, and are inefficient at low speeds. Prior gyroscope-related anti-rolling systems have either been too massive for relatively smaller vessels, such as yachts, or have been confined to use as a sensing system in combination with a structural element or elements that actually do the stabilizing. There is presently an unfilled need for an effective stabilization system deployable in boats and small ships, especially boats and small ships that are stationary or moving at low speeds.
The present invention is a machine that reduces roll motion in ships, said motion caused by waves, wakes or other disturbances. The motion is reduced by sensing the roll position and velocity, and applying a torque to counteract the forces that cause the roll motion. The counter torque is created by turning a rotating drum around a secondary axis that is normal to the drum's major spin axis. The secondary axis and the ship's roll axis are normal to one another. Conventional technology for a ship stabilizer using gyroscopic stabilization uses a flywheel with a single hub to supply the necessary angular momentum. This invention incorporates a drum supported by two or more hubs, widely spaced across the spin axis. The rotor is preferably drum shaped to balance its diameter vs. its weight vs. its angular momentum. The drum rotor is mounted in a frame, which in turn is mounted on gimbals so that the rotor can nutate under the control of the system's servo system. The servo system's operation is managed by a control system having input from the ship angular position and rate sensors.
The drum is configured to have a much higher moment of inertia than a traditional flywheel. By concentrating the mass of the drum in its outer shell or fibers, the overall weight of the drum used in this invention is less than that of the flywheel used in conventional technology, while the moment of inertia is comparable or even larger. The drum spins at a rate above 5,000 Revolutions Per Minute (RPM), and preferably spins at 10,000 RPM or higher, so the angular momentum of the rotor is much higher than that of the conventional spinning flywheel. For that reason, the rotor is made of a very lightweight metal or a non-metallic material, such as a high-strength composite material. In particular, the rotor is constructed of one or more composite materials, preferably fiber-reinforced plastic or ceramic.
With the rotor in its nominal position, the counter torque is proportional to the angular momentum of the spinning object, multiplied by the angular velocity of the entire mechanism around the secondary axis. This invention can create a larger counter roll torque than the conventional technology because the angular momentum of the machine is much larger than that of a conventional machine. Conventional technology for a ship stabilizer using gyroscopic stabilization includes a flywheel drive motor system whose speed is determined by a constant voltage. This invention uses motor controlled by an active servo system. The active control system reduces the time required for the drum to spin up to operating speed and to spin down to a full stop, when compared to the times that would be obtained using a constant voltage drive motor.
Conventional technology for a ship stabilizer using gyroscopic stabilization includes a flywheel spinning in ambient air, and during full-speed operation most of the rotor energy loss comes from air drag. The rotating drum in this invention is enclosed in a chamber with reduced air pressure, reducing the energy required to operate the machine. This chamber also acts as a protective shroud, so that failures in the rotor will be contained in the shroud chamber.
This invention includes sensors to measure the ship roll and pitch angles and rates. This invention includes active servo control of the frame gimbal's position. The torque applied to the gimbal is generated by a servo amplifier whose input is a function of the measured ship roll and pitch angles and rates, and of the gimbal's angular position and velocity.
Conventional technology for a ship stabilizer using gyroscopic stabilization incorporates passive or semi-passive control of the gimbal's position of the rotor frame, wherein the rotation of the rotor frame around its gimbals is reduced by fluid, magnetic or drum brakes, possibly as a simple function of the ship roll angular velocity. A much larger percentage reduction in ship roll motion can be much obtained using the active control system of this invention as compared to the passive or semi-passive control system of conventional technology.
The present invention fills the need for a stabilization system that may be used to counteract rolling caused by wave and wake action. The invention is an active gyrostabilizer that fits within the dimensions of a boat or small ship and achieves reasonable stabilization under the majority of sea conditions experienced by boats and small ships. The gyrostabilizer of this invention includes a rotor rotated by a rotor motor that is actively controlled by a motor control system. As indicated, in addition to regulating and generating rotor spin, the rotor motor and the motor control system act as a rotor braking system so that the gyrostabilizer can be spun down quickly as needed. The system of the present invention also preferably includes one or more angular rate sensors and one or more inclinometers to sense the exact roll position and angular velocity. In particular, solid-state angular inclinometers and rate sensors can be used to sense the boat's motion. The active control system uses information from the sensors to drive the gimbal's servomotor to control the gyrostabilizer's gimbal angle.
The rotor/frame system preferably is mounted in the vessel to orient the rotor so that the vessel roll axis, the nominal spin axis and the gimbal axis are orthogonal. This can be accomplished in two different ways. First, by having the rotor nominal spin axis be vertical and the frame gimbal's axis be athwartships, or second, by having the rotor nominal spin axis be athwartships (side-to-side) and the frame gimbal's axis be vertical. In the first case, the vessel's roll motion primarily is converted to pitching motion, which is resisted by the long, slender nature of boats. In the second case the roll motion primarily is converted to yaw (turning) motion. As a vessel's pitching motion faces more resistance than does its yaw motion, the preferred orientation is the first case. The equations that describe the rotor motion in the first orientation case are:
Where:
This equation indicates that the rotor creates a moment (LC) that opposes the roll motion of the vessel. The angular momentum is large and fixed, so the rate of gimbal rotation can be used to control the anti-roll force. Observing the general equation, the anti-roll force becomes vanishingly small when the gimbal angle reaches −90 degrees or +90 degrees, so the active controller limits the gimbal range to avoid this condition.
The gyrostabilizer includes an active servo control system for controlling the gyroscope gimbal angle. The mass of the rotor is concentrated away from its primary spin axis to minimize weight while maximizing angular momentum. The high-speed rotor around its gimbal axis may be dampened with a passive damping system or may be controlled by an active servo system. The active servo control system for the rotor gimbal's axis may be of the PID type and may include a stepped gain function to compensate for the non-linear characteristics of the gyrostabilizer.
The details of one or more examples related to the invention are set forth in the accompanying drawings and the description below. Other features, objects, and advantages of the invention will be apparent from the description, the drawings, and the appended claims.
In reference to
In reference to
In reference to
In reference to
In reference to
In reference to
In reference to
In reference to
In reference to
A fifth embodiment of the gyrostabilizer system is the same as the first embodiment shown in
A sixth embodiment of the gyrostabilizer system is the same as the second embodiment shown in
A fourth embodiment of the drum is that the drum and supporting webs are built as one continuous component using filament-wound composite construction.
The present application claims the priority benefit of U.S. provisional patent application Ser. No. 60/509,653, filed Oct. 8, 2003, entitled “GYROSTABILIZER FOR SMALL BOATS” of the same named inventor. The entire contents of that prior application are incorporated herein by reference.
Number | Name | Date | Kind |
---|---|---|---|
769493 | Schlick | Sep 1904 | A |
769693 | Forbes | Sep 1904 | A |
874255 | Skutsch | Dec 1907 | A |
1150311 | Sperry | Aug 1915 | A |
1232619 | Sperry | Jul 1917 | A |
1236204 | Norden | Aug 1917 | A |
1475460 | Schein et al. | Nov 1923 | A |
1640549 | Lamme | Aug 1927 | A |
3576134 | Fersht | Apr 1971 | A |
4176563 | Younger | Dec 1979 | A |
5511504 | Martin | Apr 1996 | A |
5628267 | Hoshio et al. | May 1997 | A |
5778735 | Groves | Jul 1998 | A |
5839386 | Frieling et al. | Nov 1998 | A |
5873560 | Sendar, Jr. et al. | Feb 1999 | A |
6014911 | Swett | Jan 2000 | A |
6122993 | Morris et al. | Sep 2000 | A |
6262505 | Hockney et al. | Jul 2001 | B1 |
6360838 | Kulhavy | Mar 2002 | B1 |
6568291 | Inman | May 2003 | B1 |
6727616 | Gabrys et al. | Apr 2004 | B1 |
6973847 | Adams et al. | Dec 2005 | B2 |
20030029367 | Katsuya et al. | Feb 2003 | A1 |
Number | Date | Country | |
---|---|---|---|
20050076726 A1 | Apr 2005 | US |
Number | Date | Country | |
---|---|---|---|
60509653 | Oct 2003 | US |