| Valvular
    Conduit U.S. Patent No. 1,329,559 To all whom it may concern:Be it known that I, Nikola Tesla, a citizen
    of the United States, residing at New York, in the county and State of New York, have
    invented certain new and useful Improvements in Valvular Conduits, of which the following
    is a full, clear, and exact description.
 In most of the machinery universally
    employed for the development, transmission and transformation of mechanical energy, fluid
    impulses are made to pass, more or less freely, through suitable channels or conduits in
    one direction while their return is effectively checked or entirely prevented. This
    function is generally performed by devices designated as valves, comprising carefully
    fitted members the precise relative movements of which are essential to the efficient and
    reliable operation of the apparatus. The necessity of, and absolute dependence on these,
    limits the machine in many respects, detracting from its practical value and adding
    greatly to its cost of manufacture and maintenance. As a rule the valve is a delicate
    contrivance, very liable to wear and get out of order and thereby imperil ponderous,
    complex and costly mechanisms and, moreover, it fails to meet the requirements when the
    impulses are extremely sudden or rapid in succession and the fluid is highly heated or
    corrosive. Though these and other correlated facts
    were known to the very earliest pioneers in the science and art of mechanics, no remedy
    has yet been found or proposed to date so far as I am aware, and I believe that I am the
    first to discover or invent any means, which permit the performance of the above function
    without the use of moving parts, and which it is the object of this application to
    describe. Briefly expressed, the advance I have
    achieved consists in the employment of a peculiar channel or conduit characterized by
    valvular action. The invention can be embodied in many
    constructions greatly varied in detail, but for the explanation of the underlying
    principle it may be broadly stated that the interior of the conduit is provided with
    enlargements, recesses, projections, baffles or buckets which, while offering virtually no
    resistance to the passage of the fluid in one direction, other than surface friction,
    constitute an almost impassable barrier to its flow in the opposite sense by reason of the
    more or less sudden expansions, contractions, deflections, reversals of direction, stops
    and starts and attendant rapidly succeeding transformations of the pressure and velocity
    energies. For the full and complete disclosure of the
    device and of its mode of action reference is made to the accompanying drawings in which
    Figure 1 is a horizontal projection of such a valvular conduit with the top plate removed.
    Figure 2 is side view of the same in elevation. Figure 3 is a diagram illustrative of the
    application of the device to a fluid propelling machine such as, a reciprocating pump or
    compressor, and Figure 4 is a plan showing the manner in which the invention is, or may be
    used, to operate a fluid propelled rotary engine or turbine. Referring to Figure 1, 1 is a
    casing of metal or other suitable material which may be cast, milled or pressed from sheet
    in the desired form. From its side-walls extended alternatively projections terminating in
    buckets 2 which, to facilitate manufacture are congruent and spaced at equal distances,
    but need not be. In addition to these there are independent partitions 3 which are deemed
    of advantage and the purpose of which will be made clear. Nipples 4 and 5, one at each
    end, are provided for pipe connection. The bottom is solid and the upper or open side is
    closed by a fitting plate 6 as shown in Fig. 2. When desired any number of such pieces may
    be joined in series, thus making up a valvular conduit of such length as the circumstances
    may require. In elucidation of the mode of operation let
    it be assumed that the medium under pressure be admitted at 5. Evidently, its approximate
    path will be as indicated by the dotted line 7, which is nearly straight, that is to say,
    if the channel be of adequate cross-section, the fluid will encounter a very small
    resistance and pass through freely and undisturbed, at least to a degree. Not so if the
    entrance be at the opposite end 4. In this case the flow will not be smooth and continues,
    but intermittent, the fluid being quickly deflected and reversed in direction, set in
    whirling motion, brought to rest and again accelerated, these processes following one
    another in rapid succession. The partitions 3 serve to direct the stream upon the buckets
    and to intensify the actions causing violent surges and eddies which interfere very
    materially with the flow through the conduit. It will be readily observed that the
    resistance offered to the passage of the medium will be considerable even if it be under
    constant pressure, but the impediments will be of full effect only when it is supplied in
    pulses and, more especially, when the same are extremely sudden and of high frequency. In
    order to bring the fluid masses to rest and to high velocity in short intervals of time
    energy must be furnished at a rate which is unattainable, the result being that the
    impulse cannot penetrate very far before it subsides and gives rise to movement in the
    opposite direction. The device not only acts as a hinderment to the bodily return of
    particles but also, in a measure, as a check to the propagation of a disturbance through
    the medium. Its efficacy is chiefly determined; first, by the magnitude of the ratio of
    the two resistances offered to disturbed and to undisturbed flow, respectively, in the
    directions from 4 to 5 and from 5 to 4, in each individual element of the conduit; second,
    by the number of complete cycles of action taking place in a given length of the valvular
    channel and, third, by the character of the impulses themselves. A fair idea may be gained
    from simple theoretical considerations. Examining more closely the mode of
    operation it will be seen that, in passing from one to the next bucket in the direction of
    disturbed flow, the fluid undergoes two complete reversals or deflections through 180
    degrees while it suffers only two small deviations from about 10 to 20 degrees when moving
    in the opposite sense. In each case the loss of head will be proportionate to a hydraulic
    coefficient dependent on the angle of deflection from which it follows that, for the same
    velocity, the ratio of the two resistances will be as that of the two coefficients. The
    theoretical value of this ratio may be 200 or more, but must be taken as appreciably less
    although the surface friction too is greater in the direction of disturbed flow. In order
    to keep it as large as possible, sharp bends should be avoided, for these will add to both
    resistances and reduce the efficiency. Whenever practicable, the piece should be straight;
    the next best is the circular form. That the peculiar function of such a
    conduit is enhanced by increasing the number of buckets or elements and, consequently,
    cyclic processes in a given length is an obvious conclusion, but there is no direct
    proportionality because the successive actions diminish in intensity. Definite limits,
    however, are set constructively and otherwise to the number of elements per unit length of
    the channel, and the most economical design can only be evolved through long experience. Quite apart from any mechanical features of
    the device the character of the impulses has a decided influence on its performance and
    the best results will be secured, when there are produced at 4, sudden variations of
    pressure in relatively long intervals, while a constant pressure is maintained at 5. Such
    is the case in one of its most valuable industrial applications which will be specifically
    described. In order to conduce to a better
    understanding, reference may first be made to Fig. 3 which illustrates another special use
    and in which 8 is a piston fixed to a shaft 9 and fitting freely in a cylinder 10. The
    latter is closed at both ends by flanged heads 11 and 12 having sleeves or stuffing boxes
    13 and 14 for the shaft. Connection between the two compartments, 15 and 16, of the
    cylinder is established through a valvular conduit and each of the heads is similarly
    equipped. For the sake of simplicity these devices are diagrammatically shown, the solid
    arrows indicating the direction of undisturbed flow. An extension of the shaft 9 carries a
    second piston 17 accurately ground to and sliding easily in a cylinder 18 closed at the
    ends by plates and sleeves as usual. Both piston and cylinder are provided with inlet and
    outlet ports marked, respectively, 19 and 20. This arrangement is familiar, being
    representative of a prime mover of my invention, termed "mechanical oscillator",
    with which it is practicable to vibrate a system of considerable weight many thousand
    times per minute. Suppose now that such rapid oscillations
    are imparted by this or other means to the piston 8. Bearing in mind the proceeding, the
    operation of the apparatus will be understood at a glance. While moving in the direction
    of the solid arrow, from 12 to 11, the piston 8 will compress the air or other medium in
    the compartment 16 and expel it from the same, the devices in the piston and head 11
    acting, respectively, as closed and open valves. During the movement of the piston in the
    opposite direction, from 11 to 12, the medium which has meanwhile filled the chamber 15
    will be transferred to compartment 16, egress being prevented by the device in head 12 and
    that in the piston allowing free passage. These processes will be repeated in very quick
    succession. If the nipples 4 and 5 are put in communication with independent reservoirs,
    the oscillations of the piston 8 will result in a compression of the air at 4 and
    rarefaction of the same at 5. Obviously, the valvular channels being turned the other way,
    as indicated by dotted lines in the lower part of the figure, the opposite will take
    place. The devices in the piston have been shown merely by way of suggestion and can be
    dispensed with. Each of the chambers 15 and 16 being connected to two conduits as
    illustrated, the vibrations of a solid piston as 8 will have the same effect and the
    machine will then be a double acting pump or compressor. It is likewise unessential that
    the medium should be admitted to the cylinder through such devices for in certain
    instances ports, alternately closed and opened by the piston, may serve the purpose. As a
    matter of course, this novel method of propelling fluids can be extended to multistage
    working in which case a number of pistons will be employed, preferably on the same shaft
    and of different diameters in conformity with well established principles of mechanical
    design. In this way any desired ratio of compression or degree of rarefaction may be
    attained. Fig. 4 exemplifies a particularly
    valuable application of the invention to which reference has been made above. The
    drawing shows in vertical cross section a turbine which may be of any type but is in this
    instance one invented and described by me and supposed to be familiar to engineers.
    Suffice it to state that the rotor 21 of the same is composed of flat plates which are set
    in motion through the adhesive and viscous action of the working fluid, entering the
    system tangentially at the periphery and leaving it at the center. Such a machine is a
    thermodynamic transformer of an activity surpassing by far that of any other prime mover,
    it being demonstrated in practice that each single disk of the rotor is capable of
    performing as much work as a whole bucket-wheel. Besides, a number of other advantages,
    equally important, make it especially adapted for operation as an internal combustion
    motor. This may be done in may ways, but the simplest and most direct plan of which I am
    aware is the one illustrated here. Referring again to the drawing, the upper part of the
    turbine casing 22 has bolted to it a separate casting 23, the central cavity 24 of which
    forms the combustion chamber. To prevent injury through excessive heating a jacket 25 may
    be used, or else water injected, and when these means are objectionable recourse may be
    had to air cooling, this all the more readily as very high temperatures are practicable.
    The top of casting 23 is closed by a plate 26 with a sparking or hot wire plug 27 and in
    its sides are screwed two valvular conduits communicating with the central chamber 24. One
    of these is, normally, open to the atmosphere while the other connects to a source of fuel
    supply as a gas main 28. The bottom of the combustion chamber terminates in a suitable
    nozzle 29 which consists of a separate piece of heat resisting material. To regulate the
    influx of the explosion constituents and secure the proper mixture of air and gas conduits
    are equipped, respectively, with valves 30 and 31. The exhaust openings 32 of the rotor
    should be in communication with a ventilator, preferably carried on the same shaft and of
    any suitable construction. Its use, however, while advantageous, is not indispensable the
    suction produced by the turbine rotor itself being, in some cases at least, sufficient to
    insure proper working. This detail is omitted from the drawing as unessential to the
    understanding. But a few words will be needed to make
    clear the mode of operation. The air valve 30 being open and sparking established across
    terminals 27, the gas is turned on slowly until the mixture in the chamber 24 reaches the
    critical state and is ignited. Both the conduits behaving, with respect to efflux, as
    closed valves, the products of combustion rush out through the nozzle 29 acquiring still
    greater velocity by expansion and, imparting their momentum to the rotor 21, start it from
    rest. Upon the subsidence of the explosion the pressure in the chamber sinks below the
    atmosphere owing to the pumping action of the rotor or ventilator and new air and gas is
    permitted to enter, cleaning the cavity and channels and making up a fresh mixture which
    is detonated as before, and so on, the successive impulses of the working fluid producing
    an almost continuous rotary effort. After a short lapse of time the chamber becomes heated
    to such a degree that the ignition device may be shut off without disturbing the
    established regime. This manner of starting the turbine involves the employment of an
    unduly large combustion chamber which is not commendable from the economic point of view,
    for not only does it entail increased heat losses but the explosions cannot be made to
    follow one another with such rapidity as would be desirable to insure the best valvular
    action. When the chamber is small an auxiliary means for starting, as compressed air, may
    be resorted to and a very quick succession of explosions can then be obtained. The
    frequency will be the greater the stronger the suction, and may, under certain conditions,
    reach hundreds and even thousands per second. It scarcely need be stated that instead of
    one several explosion chambers may be used for cooling purposes and also to increase the
    number of active pulses and the output of the machine. Apparatus as illustrated in Fig. 4 presents
    the advantages of extreme simplicity, cheapness and reliability, there being no
    compressor, buckets or troublesome valve mechanism. It also permits, with the addition of
    certain well known accessories, the use of any kind of fuel and thus meets the pressing
    necessity of a self-contained, powerful, light and compact internal combustion motor for
    general work. When the attainment of the highest efficiency is the chief object, as in
    machines of large size, the explosive constituents will be supplied under high pressure
    and provision made for maintaining a vacuum at the exhaust. Such arrangements are quite
    familiar and lend themselves so easily to this improvement that an enlargement on this
    subject is deemed unnecessary. The foregoing description will readily
    suggest to experts modifications both as regards construction and application of the
    device and I do not which to limit myself in these respects. The broad underlying idea of
    the invention is to permit the free passage of a fluid through a channel in the direction
    of the flow and to prevent its return through friction and mass resistance, thus enabling
    the performance of valve functions without any moving parts and thereby extending the
    scope and usefulness of an immense variety of mechanical appliances. I do not claim the methods of an apparatus
    for the propulsion of fluids and thermodynamic transformation of energy herein disclosed,
    as these will be made subjects of separate applications. I am aware that asymmetrical conduits have
    been constructed and their use proposed in connection with engines, but these have no
    similarity either in their construction or manner of employment with my valvular conduit.
    They were incapable of acting as valves proper, for the fluid was merely arrested in
    pockets and deflected through 90 degrees, this result having at best only 25% of the
    efficiency attained in the construction herein described. In the conduit I have designed
    the fluid, as stated above, is deflected in each cycle through 360 degrees, and a
    co-efficient approximating 200 can be obtained so that the device acts as a slightly
    leaking valve, and for that reason the term "valvular" has been given to it in
    contrast to asymmetrical conduits, as heretofore proposed, which were not valvular in
    action, but merely asymmetrical as to resistance. Furthermore, the conduits heretofore
    constructed were intended to be used in connection with slowly reciprocating machines, in
    which case enormous conduit-length would be necessary, all this rendering them devoid of
    practical value. By the use of an effective valvular conduit, as herein described, and the
    employment of pulses of very high frequency, I am able to condense my apparatus and secure
    such perfect action as to dispense successfully with valves in numerous forms of
    reciprocating and rotary engines. The high efficiency of the device,
    irrespective of the character of the pulses, is due to two causes: first, rapid reversal
    of direction of flow and, second, great relative velocity of the colliding fluid columns.
    As will be readily seen each bucket causes a deviation through an angle of 180 degrees,
    and another change of 180 degrees occurs in each of the spaces between two adjacent
    buckets. That is to say, from the time the fluid enters or leaves one of the recesses to
    its passage into, or exit from, the one following a complete cycle, or deflection through
    360 degrees, is effected. Observe now that the velocity is but slightly reduced in the
    reversal so that the incoming and deflected fluid columns meet with a relative speed,
    twice that of the flow, and the energy of their impact is four times greater than with a
    deflection of only 90 degrees, as might be obtained with pockets such as have been
    employed in asymmetrical conduits for various purposes. The fact is, however, that in
    these such deflection is not secured, the pockets remaining filled with comparatively
    quiescent fluid and the latter following a winding path of least resistance between the
    obstacles interposed. In such conduits the action cannot be characterized as
    "valvular" because some of the fluid can pass almost unimpeded in a direction
    opposite to the normal flow. In my construction, as above indicated, the resistance in the
    reverse may be 200 times that in the normal direction. Owing to this a comparatively very
    small number of buckets or elements is required for checking the fluid. To give a concrete
    idea, suppose that the leak from the first element is represented by the fraction 1/X,
    then after the nth bucket is traversed, only a quantity (1/X)n will escape and it is
    evident that X need not be a large number to secure a nearly perfect valvular action. What I claim is:1. A valvular conduit having interior walls
    of such conformation as to permit the free passage of fluid through it in the direction of
    flow, but to subject it to rapid reversals of direction when impelled in the opposite
    sense and thereby to prevent its return by friction and mass resistance.
 2. A valvular conduit composed of a closed
    passageway having recesses in its walls so formed as to permit a fluid to pass freely
    through it in the direction of flow, but to subject it to rapid reversals of direction
    when impelled in an opposite sense and thereby interpose friction and mass resistance to
    the return passage of the same. 3. A valvular conduit composed of a tube or
    passageway with rigid interior walls formed with a series of recesses or pockets with
    surfaces that reverse a fluid tending to flow in one direction therein and thereby check
    or prevent flow of the fluid in that direction. 4. A valvular conduit with rigid interior
    walls of such character as to offer substantially no obstacle to the passage through it of
    fluid impulses in one direction, but to subject the fluid to rapid reversals of direction
    and thereby oppose and check impulses in the opposite sense. 5. A valvular conduit with rigid interior
    walls formed to permit fluid impulses under pressure to pass freely through it in one
    direction, but to subject them to rapid reversals of direction through 360 degrees and
    thereby check their progress when impelled in the opposite sense. 6. A valvular conduit with rigid interior
    walls which permit fluid impulses to flow through it freely in one direction, formed at a
    plurality of points to reverse such fluid impulses when impelled in the opposite direction
    and check their flow. 7. A valvular conduit with rigid interior
    walls having pockets or recesses, and transversely inclined intermediate baffles to permit
    the free passage of fluid impulses in one direction but to deflect and check them when
    impelled in the opposite direction. In testimony whereof I affix my signature Nikola Tesla |