Howell Torpedo Co. v. E. W. Bliss Co.
Opinion of the Court
This suit involves the construction and infringement by defendant of claim i of letters patent No. 311,325, issued to Admiral John A. Howell on January 27, 1895, for “certain new and useful improvements in marine torpedoes.” Claim 1 is as follows:
“(3) The combination, with the torpedo case or shell and the fly wheel mounted therein, with its rotation axis located substantially as described, to of)tain a resultant axis of motion in case of deviating forces acting on the torpedo, of steering mechanism, and suitable devices for controlling the same, arranged and operating substantially in the manner hereinbefore set forth, whereby said steering mechanism shall be brought into action upon occurrence of the resultant motion, and when thus brought into action shall be caused to set up an opposite deviating- force, which will counteract and neutralize the initial extraneous deviating force.”
It seems to be undoubted that Admiral Howell was the first person to suggest and to use a rapidly revolving fly wheel in a marine torpedo (1) to preserve fixity of direction, (2) to steer the 'torpedo against the influence of deviating forces. The conception of both purposes is embodied in the letters patent mentioned, and of the first use iti letters patent issued to the same inventor in 1871. The conception of this double use was the beginning of the art, and from it has sprung all essential knowledge respecting the directing and steering of torpedoes, although different and better details in the mechanisms employed have been devised by others. Although the merit of the primary conception that fixity of direction and ability to steer marine torpedoes could be acquired by the use oí a revolving fly wheel adjusted in the torpedo is due to Admiral Howell, the conclusion cannot be escaped that claim 1 limits the use of the art- so, created and developed by the inventor, as regards steering, to steering mechanism brought into action by resultant motion, and that the letters show 110 appreciation of the steering mechanism employed by( the defendant. The discussion can proceed clearly only by a description of the device known as a “gyroscope” and an explanation of its phenomena; for, although he does not seem to have identified specifically his proposed mechanism with the gyroscope, nor, at the outstart at least, to have understood that he was utilizing the laws, of that instrument, yet the fly wheel proposed to be used by Admiral Howell in the torpedo, in connection with the torpedo’s outer shell and the water, is in fact a gyroscope, and obeys its laws. If a swiftly revolving fly wheel be adjusted so that its axis is free to take .any direction, its axis, in absence of external disturbing forces, will, remain nearly invariable in direction. This, following the descriptive articles, may be called “the stability of direction oí the axis of rotation.” The fly wheel persists in rotating in the given direction, and so its axis tends to resist any deflecting influence. The gyroscope proper usually is constructed by placing the fly wheel so that it may rotate inside a circular ring around its shorter axis, the axis running
“It consists of a fly -wheel, with a heavy rim accurately turned and Balanced, which can rotate round an axis, GO, forming a diameter of the ring,' I-C This ring also can rotate about the axis, AF, which is at right angles to GO, and is a diameter of the ring, L. Similarly, this ring. L, can rotate about the vertical axis, BH, which is perpendicular both to GO and AF, and forms a diameter of the ring, M, which is screwed to the heavy sole plate, N.”
The fly wheel is free to move on its own axis or that of either ring, but will not move on the latter, while the wheel is rotating rapidly, in the absence of a deviating force; that is, the tendency of the revolving wheel is to keep-the rings stationary. However, when some force other than that impelling the fly wheel is brought to bear on either of the rings, it will cause the fly wheel to turn on the axis of the inner ring, or the axis of the outer ring, or both, accordingly as the force may be applied, pursuant to the law that “a body actuated by several forces moves in the direction of their resultant.” If now it be shown that in practice the presence of one resultant motion brings into play the complainant’s steering mechanism, the meaning of claim i may be understood. The specification represents the axis of the fly wheel as transverse to the torpedo, although it states that such axis may be placed longitudinally, but no steering mechanism fop the second location is described or suggested. But .by placing the axis transversely, its ends are supported in the shell of the torpedo. In its simplest form this is shown as follows:
*909
Here the sides of the torpedo form the first or inner ring, in which the axis of the fly wheel is located in the gyroscope shown above. The outer ring is absent; but as the water allows the fly wheel, when disturbed, to tip on a vertical axis, and also to either side with lateral motion of the torpedo, the freedom of motion permitted in a gyroscope is attained. So, also, there are attained the resultant motions observed when extrinsic forces come in contact with the rings of the gyroscope. The only resultant motion that is employed by Admiral Howell in claim i is that which may take place on the axis of the inner ring of the gyroscope as shown, which corresponds to the longitudinal axis of the torpedo; or, in short, it is the motion of the torpedo rolling on one of its sides. The cause and nature of that lateral rolling are shown by the following figure:
If, as shown, the deflecting force be applied at the starboard bow of the torpedo while the fly wheel is revolving from right to left, looking at the torpedo from that side, the torpedo will roll to port under the influence of the fly wheel made fast to its sides; that is, a new force combined wfith the existing force operating the fly wheel results in rolling the torpedo sideways, thereby elevating the starboard side and lowering the port side. It is not worth while to try to trace the cause. It is enough that this is the exact law of the gyroscope when subjected to a similar foreign force, and, of course, the result would not be attained except for the presence of a gyro
*911 “Tlie steering mechanism will now bo described. I make use of two steering rudders, O, in the present instance, although J may use one only, or even more than two, if desired. These rudders are vertical, and turn on vertical posts or axes, g, in tlie framework, f, and are arranged one on each side of (.lie after portion of rear section, E. Each of them is slotted, as indicated by dotted lines in Fig. 7, so that it will straddle the adjoining propeller shaft and framework, and be free to move without interfering with the latter. These rudders are by arms, li, and links or rods, i (which latter pass through tubes, 1', in the water-tight part of section E, into the forward ojien part of said section), connected to opposite ends of a centrally pivoted lever, j, whose axle is provided with a radial arm, j', connected by a link, j2, to a crank arm, k2, on the axle, k'. of the tiller, k. Under this arrangement it will be seen that botli rudders can, by moving the tiller, bo moved to starboard or port or be brought midships, as occasion may demand. The automatic action of the tiller for this purpose is brought about as follows: On one of the propeller shafts G, is a worm, 1, Fig. (i, which gears with and drives a wheel, i£, mounted on a vertical'axle, in', in the open part of section E, and on the same axle is fixed a wheel, H', having- a cam rib, m, on its upper face. The axle revolves continuously so long as the propeller shaft revolves. The tiller, k, overhangs the cam wheel FI', and at its outer end carries a pivoted arm, li. arranged crosswise of the torpedo, tlie axle, n', of which Is hung in ears or bearings on tlie under side of the outer end of the tiller, and is connected l>y means of a flexible shaft, o,—for instance, a shaft of closely coiled wire, •—to the axle, p', of a pendulum, p, as indicated in Figs. 0 and 7. The axle, n', of the arm, n, is horizontal, and extends in the direction of the length of rhe torpedo, and the axis of the pendulum is on the prolongation of it The arm, n, at its ends lias points, n2, one or the other of which will engage the cam wheel whenever the latter is inclined laterally in one direction or the other relatively to the arm. The operation of the parts is as follows: The pendulum, p, tends1 to keep the points, n2, of the arm, n, always in a horizontal plane, and the cam wheel normally lies in a plane parallel thereto. With tlie parts in this position, the tiller is midships, as represented in the drawings; but whenever, by an extraneous deflecting force, tlie torpedo is caused to roll upon its longitudinal axis in one direction or tlie oilier, the cam wheel is tilted or inclined in a corresponding direction with reference to the arm, n, which, hy its pendulum, is maintained horizontal. Consequently the continuously revolving cam wheel is thrown into engagement with one or tlie other of the points, n2, of tlie arm, with the result of putting the helm to port or starboard, as tlie case may be, the flexible shaft, o, permitting this movement. Tlie steering rudders, when thus moved, set up a deflecting force opposed to the initial extraneous deflecting force, with the result of producing in the torpedo a tendency to roll in the opposite, direction, tlie helm being-put to starboard when the torpedo rolls to starboard, and vice versa. This action will continue until the rudders have rolled the torpedo back far enough to permit the disengagement of the arm, n, and cam wheel; or, in other words, until tlie cam wheel is in its normal horizontal position, in this way it will he seen that tlie torpedo can be automatically steered or kept from leaving the course in which it was pointed at the time it was launched. The rudders are not simply turned to starboard or port, as the case may be, and held there until the torpedo is brought hack to its course. The revolving cam wheel imparts to them a series of Impulses, and this is kept up so long ns tlie tilting arm engages the cam wheel. The cam rib may be so formed as to impart one or more impulses to the rudder or rudders for each revolution.”
Tt will be observed that under tlie intended ad ion of tlie mechanism duly operating- the torpedo is automatically righted or "restored to equilibrium, and that this is effected with such quickness that the torpedo is not expected to deflect from its course, or at least the deflection is quickly arrested. The result is that the rudders do not directly steer the torpedo from one direction to another, but in the first instance restore the level of the torpedo; for the deviating force
“The gist of my invention, so far as concerns the correcting of deviations in the course of the torpedo, lies in so placing the rotation axis of the fly wheel as to obtain a resultant axis of motion in the ease of deviating forces acting on the torpedo, and in combining with the fly wheel thus placed mechanism, termed by me ‘steering mechanism,’ brought into action by the resultant motion, and arranged and automatically operating to set up an. opposite deviating force which will'counteract and neutralize the initial extraneous deviating force.”
This language is most fortunate to express concisely what is stated with great particularity in other parts of the specification, and describes without other reference that part of claim i which relates to steering the torpedo. Before considering claim x, something may be said briefly about the words “resultant axis of motion,” which occur in such claim, as well as in the language quoted above. The scientists connected with the case have disputed concerning the meaning of the phrase, quite unnecessarily for a fair understanding, of the inventor’s meaning. Admiral Howell states:
“In the patent specification I have used the terms ‘resultant axis’ and ‘resultant axis of motion’ meaning by these, not the axis of the fly wheel, or any position which this axis may assume, but that line or axis about which the axis of the fly wheel swings in tilting, due to the action of a deviating force. Thus, if the fly wheel is rotating, and the deflecting force is applied-tending to tilt its axis, this axis will tilt, but in a direction approximately 90° from the direction of the deflecting force, and the line about which the whole wheel tilts will be the resultant axis of motion. In the Howell torpedo, with the fly wheel arranged transverse and horizontal, a deflecting force will cause the axis of the fly wheel to tilt up about a line running longitudinally through the torpedo, and this line will be the resultant axis of motion about- which the axis of the fly wheel tilts.”
Again, he states:
>“I use axis in the ordinary sense as the line about which motion takes place, and by ‘resultant axis’ I mean that axis about which the resultant motion takes place.”
Fig. 4 shows the gyroscopic wheel as supported in the torpedo, so that its axis is free to move in any direction relatively to any point of the torpedo. The axis, a, a, is pointed at the target, and is parallel with the longitudinal axis of the torpedo. If now a deviating force deflect the longitudinal axis of the torpedo to c, c, yet the axis, a, a, of the wheel will remain pointing as before, and the oiiter gimbal ring will maintain its position. The control pin, d, is set vertically in the outer gimbal ring, within the fork of the valve arm, e. If the bow of the torpedo be deflected to port, throwing the stern to starboard, the forked arm will engage the control pin in the outer gimbal ring on account of the motion of the torpedo, and the steering gear will be set in operation, so that the rudder will tend to swing the torpedo back into its course. If it should swing back so that its axis goes
“Under tliese conditions the axis of resultant rotation, or motion due to 1lio application of a laterally deflecting- force, will be the longitudinal axis of the torpedo,-—in other words, the torpedo will roll; and this rolling can be convoumntly availed of to bring into action steering mechanism arranged and operating" to apply automatically an opposite deflecting or deviating force, which will restore the status quo. As soon as the rolling ceases, the steering mechanism becomes inactive; but until then it constantly offers to the <i(--fleeting force an opposition which in the end overcomes and suppresses it.”
Complainant was understood on the argument to contend that, as the stability of either ring in a gyroscope can be possible only when resultant motion is possible, the stability of the ring is traceable to resultant motion. Stability is not the effect of resultant motion, nor is it dependent upon it. Stability of the rings depends solely upon the rotation of the fly wheel undisturbed by friction or extraneous forces, and is the normal condition of the gyroscope in operation. On the other hand, resultant motion is error, fortuitous and undesired rotation of the fly wheel on a second axis, the revolution of a ring, all produced by the introduction of a new force foreign to that under which the fly wheel was operating. The Whitehead steering gear depends upon fixity of axis, and rings, unaffected by an extrinsic
The complainant’s bill must be dismissed, with costs.
Case-law data current through December 31, 2025. Source: CourtListener bulk data.