Method and apparatus for continuously suppressing unwanted rotational phenomena in a rotating body

• US 5,099,430 A
• Filed: 10/28/1988
• Issued: 03/24/1992
• Est. Priority Date: 10/28/1988
• Status: Expired due to Fees

• Current Assignee: Joseph Hirsch
• Original Assignee: Joseph Hirsch
• Inventors: Hirsch, Joseph
• Primary Examiner(s): Gruber, Felix D.
• Application Number:
  US07/264,136
• Time in Patent Office: 1,243 Days
• Field of Search: 364/508, 73/462-469, 73/659, 73/660
• US Class Current: 73/462
• CPC Class Codes: F16F 15/31 characterised by means for varying the moment of inertia
• CPC Class Codes: F16F 15/322 the rotating body being a shaft F16F15/34, F16F15/36 take precedence
• CPC Class Codes: G01M 1/34 by removing material from the body to be tested, e.g. from the tread of tyres

Abstract

For a body rotating on an axis and having a moment of inertia relative to the axis, an apparatus for dynamically suppressing unwanted rotational phenomena occurring relative to the axis of rotation, i.e., phenomena which exhibit themselves in a body only when the body is rotating about the axis, such as, dynamic imbalance and resonance at critical rotational speeds. One or more inertial masses are movably affixed to the body such that they can be selectively moved radially and circumferentially with respect to the axis. Appropriately placed sensors, such as strain gauges, accelerometers, vibration transducers, and the like detect the phenomena and pass pertinent parameters of the phenomena to a controller, preferably a computer, which analyzes the parameters to determine, among other things, the magnitudes of the phenomena. If a magnitude exceeds a selected threshold, the controller determines the optimum positions for one or more of the movable inertial masses to eliminate or effectively suppress the respective phenomenon.

Claims

1. For a body rotating on an axis and having a moment of inertia relative to said axis, a system for dynamically suppressing dynamic imbalance of said body relative to said axis of rotation, comprising:

(a) means for selectively varying the magnitude and phase of the moment of inertia of said rotating body relative to said axis of rotation in at least one pair of radial planes on opposite sides of the center of mass of the rotating body while said body is in-place and rotating, said means for varying the moment of inertia being responsive to control signals,

(b) means for sensing a condition of imbalance with respect to said axis of rotation, and for communicating pertinent parameters of said sensed imbalance to a control means,

(c) the control means comprising;

(1) means responsive to parameters communicated by the sensing means for selecting trial and imbalance correction variations in the magnitude and phase of the moment of inertia of the rotating body, and

(2) means for producing said control signals corresponding to said selected variations in the magnitude and phase of the moment of inertia of said rotating body.

2. The system according to claim 1 wherein the means for varying the magnitude and phase of the moment of inertia in said pair of radial planes comprises:

(a) two known masses movably affixed to the rotating body, one in each of said radial planes, and

(b) means for selectively and individually moving said known masses radially and angularly, both with respect to the axis of rotation, within their respective planes.

3. The system according to claim 1 wherein said means responsive to parameters communicated by the sensing means for selecting trail and imbalance correction variations is a computer executing the set of programs comprising the software in the IRD Model #245 Balancer or their equivalent adapted for automatic operation.

4. The system according to claim 1 wherein the means for varying the magnitude and phase of the moment of inertia in said pair of radial planes comprises:

(a) at least two pairs of known masses, the pairs being disposed on opposite sides of the center of mass of the rotating body in respective planes normal to the axis of rotation of the body,

(b) for each known mass of each pair, means for driving said mass bi-directionally along a radial line of movement, with respect to the axis of rotation, in said mass'"'"' respective plane, and holding said mass at selected positions on said line of movement, the lines of movement of the known masses of each pair being spaced angularly apart, and

(c) for each pair, means for selectively coupling and decoupling rigidly both driving means of said pair from the rotating body in order to selectively set the phase of the couple of the pairs.

5. The system according to claim 4 wherein the means for driving each known mass bi-directionally along a radial line of movement and holding said mass at selected positions on said line of movement comprises a screw shaft upon which the mass is threaded being steppingly turned by a stepper motor, and means for selectively energizing the stepper motors.

6. The system according to claim 4 wherein the means for selectively coupling and decoupling rigidly both driving means of each pair of known masses from the rotating body comprises:

(a) an annular electromagnetic means affixed to an axial shaft protruding from the rotating body,

(b) a ring slippingly mounted concentrically upon the annular electromagnetic means, the driving means being mounted upon the annular ring, the annular ring being held in rigid relation to the electromagnetic means when the electromagnetic means is energized, and

(c) means for selectively energizing said electromagnetic means.

7. For a rotating body having at least two known massed movably affixed to the rotating body on opposite sides of the center of mass of the rotating body, the masses being selectively and individually movable radially over a range and angularly over substantially 360 degrees, both with respect to the axis of rotation of the body, a method of achieving in-place dynamic balance of the body with respect to the axis of rotation of said body while it is rotating, comprising the steps:

(a) positioning at least two force measuring devices in positions on opposite sides of the center of mass of said body where they can each measure, at their respective positions, the dynamic forces exerted by the body with reference to the axis of rotation,

(b) comparing the respective force measurements of said devices to determine if a dynamic imbalance exists,

(c) if an imbalance exists, comparing the magnitude of the imbalance with a pre-selected threshold value,

(d) if an imbalance exists and its magnitude exceeds the threshold value, determining a trial variation of the magnitude and phase of the moment of inertia of the body,

(e) moving at least one of the known masses in its respective radial plane of movement to affect the trail variation,

(f) noting all changes and/or absence of changes in the dynamic forces being measured,

(g) returning the mass moved for the trial variation to its original position,

(h) calculating from the noted changes and/or absence of changes the respective radial and angular positions at which the known masses would offset the imbalance, and

(i) moving the known masses to their respective calculated positions.

8. For a rotating body having at least two known masses movably affixed to the rotating body on opposite sides of the center of mass of the rotating body, the masses being selectively and individually movable radially over a range and angularly over substantially 360 degrees, both with respect to the axis of rotation of the body, a method of maintaining in-place dynamic balance of the body with respect to the axis of rotation of said body while it is rotating, comprising the steps:

(a) positioning at least two force measuring devices in different positions on opposite sides of the center of mass of said body where they can each measure, at their respective positions, the dynamic forces exerted by the body with reference to the axis of rotation,

(b) continuously comparing the respective force measurements of said devices to determine if a dynamic imbalance exists,

(c) if an imbalance exists, comparing the magnitude of the imbalance with a pre-selected threshold value,

(d) if an imbalance exists and its magnitude exceeds the threshold value, determining a trial variation of the magnitude and phase of the moment of inertia of the body,

(e) if an imbalance exists and its magnitude does not exceed the threshold value, then repeating step (b),

(f) moving at least one of the known masses in its respective radial plane of movement to affect the trial variation,

(g) noting all changes and/or absence of changes in the dynamic forces being measured,

(h) returning the mass moved for the trial variation to its original position,

(i) calculating from the noted changes and/or absence of changes the respective radial and angular positions at which the known masses would offset the imbalance,

(j) moving the known masses to their respective calculated positions, and

(k) repeating step (b).