US2242638A - Light control means - Google Patents

Description

ay 0, 1941. .1. R. BALSLEY 2,242,638

LIGHT CONTROL MEANS- Filed July 10, 1940 INVENTOR. Jiunes RBalsley Patented May 20, 1941 LIGHT CONTROL MEANS 'James R. Balsley, Stamford, Conn, assign'or, by

direct and mesne assignments, to James R.

SEP 3 (3 "i911 Balsley, Incorporated, Stamford, Conn, a corporation of Connecticut Application July 10, 1940, Serial No. 344,706

15 Claims. ,(Cl. 250-415) The present invention relates to means for controlling the stabilizing electrically energized light sources. Particularly the invention relates to means for stabilizing such light sources through the use of what may be termed optical feedbac In numerous instances, such as photoengraving, printing of photographic film and the like, it is necessary that a light source of uniform intensity be utilized. While many attempts have been made to achieve this aim through the regulation of the supply voltage, such attempts have not been successful since they do not compensate for variations in light intensity resulting from usage of the equipment.

For example, when an incandescent lamp is the light source no maintenance of the voltage at a constant value can compensate for the deterioration of the filament or blackening of the glass by depositing of the filament material thereon which occurs as a natural result of the use of the lamp. Further, in instances in which lamps of the mercury vapor type are used, the maintenance of the supply voltage at a constant value is entirely inadequate. Light intensity is a function of power which is the. product of voltage and current. The ratio of current to voltage is a function of the gas pressure which is, in turn, a function of temperature. As an example, a particular lamp may take 0.4 ampere at 250 volts under certain conditions and, by subjectingthe burner to a blast of cold air, be made to dissipate the same amount of energy with a current of 0.8 ampere at 125 volts. It is obvious that, if the voltage is maintained at a constant value, the intensity will change with changes in temperature.

Moreover, lamps of the low pressure mercury vapor type have notbeen suitable to uses which involve modulation of the lamp, such, for example, as sound-on-film recording and light signalling, due to the fact that the random vaporization and condensation. of mercury particles in the are create variations in light intensity of suchmagnitude and frequency that they interfere seriously with the recording or signalling. The present invention, on the other hand, supplies the light source with its energizing current through the medium of an electron discharge tube, the lamp in turn being caused to shinev upon a photo-electric cell which is in a. circuit such that the output of the cell is fed back to the electron discharge tube and controls the gain of that tube. By this means the intensity of the light itself controls the operation .of the circuit so that the intensity is maintained constant or is modulated in exact accordance with the signal to be converted into light.

An object of the invention is to provide a light source which will be of uniform intensity in the presence of conditions which would'normally tend to change the intensity at rates varying between zero and many thousands of cycles per second.

A further object of the invention is to provide such uniform intensity light through the .medium of a system in which the light source itself controls the supply of energy thereto.

It is a further object of the invention to provide a means whereby a light source may be modulated without'bringing about disturbances which alter the intensity of the light in accordance with factors other than the modulation.

Other objects and features .of the invention will be set forth in connection with the following description when considered in connection with the appended drawing, in which,

Figure 1 is a diagram of a circuit for maintaining constant intensity of a light source;

Figure 2 is a diagram of a circuit similar. to that Q l of Figure 1, in which, however, only a portion of the current to the light source is supplied through an electron discharge tube, the greater portion being supplied by a generator;

Figure 3 is a diagram of the circuit illustrating the modulation of a light source in such aman ner that its intensity is varied in accordance with the modulation only without the interposing of any foreign disturbances; and

Figured is a diagram of the application of the circuit of Figure 1 to the problem of copying photographs, documents, and the like, making an exact copy as regards density and contrast or any desired variation of either or both irrespective of the latent contrast of the copy paper or film being used.

Referring to Figure 1, there is at it a battery or other current source which supplies plate current to an electron discharge tube H, which tube is in the circuit of a light source l2. Placed near the light source it is a photo-electric cell 83 and between the two is a shutter It, by means of which the amount of light falling on the photo-electric cell'from light source l2 may be adjusted.

The plate and grid of tube H are connected by I terminalofcurrentsource lflandtomakethis potential substantially independent of the oathode current of tube l6. In order to keep the a compensation as described above is of great practical value. g

It has further been found that when such mercury vapor lamps are used in the conventional variation in current through tube II as small as .met the intensity may be reduced to about possible, it is supplied. with additional current thromh resistance l8. shunting the tube i1 is a resistance 20, having an addustable tap which is connected through a resistance ill, or a portion resistance 2| to the photo-electric cell It Resistance 20 is large as compared with the resistance of tube i1 and small as compared with resistance 2|, which latter is the principal load re-,

sistance {or photo-electric cell 13. Resistance ii may be used to supply a steady current to light source I2 by shunting tube ii for a purpose to be described later.

.The circuit above described is a two-stage amplifier of the so-called D. C. type, driven by a photo-electric cell and; consisting of one voltage amplifier stage and one power stage with the lamp 12 as load for the power stage.

In operation, the light intensity is adjusted by regulating the grid voltage of tube It. This may be effected in either of two ways or by a combination thereof. One of the two ways of adjust-p ing is by regulating the amount of light reaching cell l3, as for example by regulating the aperture in diaphragm or shutter l 4. The other mode of adjusting is by regulating the'position of the adjustable taps on resistances 20 and 2|.

It will be seen that if the light intensity tends to increase, current from photo-electric cell I! will increase and will cause an increased flow 3 of current thro h the resistance 2| and consequentlycause e grid of tube lite become more positive. This in turn will cause an increased flow of current throughtube l6 and flow of current through resistance l5, thus causing the grid of tube. I I to become more negative,

thereby reducing the energizing current for lamp J II. of course, in-a similar manner, it the light intensity tends todecrease, the resulting increase or the energizing current for lamp I! will ccmpensate for this tendency.

As an illustration of the practical advantage of the, invention and the manner Inwhichit operates, an experiment utilizing a G. E. type H3 mercuryvaporlampwillbedescribed. 'il'hislarnp, 59

conditions, the shutter ll, which had been closed,

was suddenly opened, thereby adjusting the light intensity to a new and lower value. The intensity decreased instantly, the voltage on the tube rising rapidly to approximately 255 volts and the eminent dropping to 0.1 ampere. During the ensuing several minutes, while the lamp was reaching its'new point of thermal equilibrimn, the voltage slowly droppedto approximately 125.

and the current slowly rose to approximately 35 0.2 ampere, with absolutely no change in intensity during the entire period. In other words,

the control means of this invention automatically pplied the needed current to maintain uniform-- intensity as the voltage across the lamp varied as a function of the slowly changing internal temperatureandpressure .It will be'obvious that since air currents on a lampot'thistypecreatelargechangesintempenattire-and consequent pressure, such '75 thirty per cent of its normal value by reducing the voltage across the lamp. when the voltage is reduced further, the arc breaks and, the light is extinguished. thereof, to the grid of tube l6, and also through 10 By the means disclosed, the intensity may be reduced to less than oneper cent of its normal intensity either slowly or periodically and the arc is found to be entirely stable.

For uses where the disturbances which tend to alter the intensity represent depths of modulation which are appreciably less than one hundred per cent, that portion of the current which will be considered as the steady current may be supplied by a battery, by a resistance shunting tube ll as-shown in Figure 1 or by a generator.

The portion of current required to for disturbances may be supplied through an electron discharge tube as previously described. Figure 2 shows a circuit utilizing a generator for the pu p se mentioned, and also tor performing another function, that of compensating automatically for slow variations in intensity even ,of great amplitude as will be described later. As an illustration of the operation of this circuit, particular values are The lamp l2 draws 1.2 amperes at 840 volts. When operated on direct current it is discovered that it is subject to high frequency variations; amounting to thirty per cent maximum modulation. The modulation current is then 0.3 times 1.2 amperes, or 0.38 ampere.

A generator represented as having armature 30 and held windings and 82' will su'PDly'the lamp with 0.84 ampere at 840 volts. Field winding ll is wound to operate in the plate circuit of tube i I to take 0.38 ampere normally. It is so connected that as the current through it increases the butput voltage of the generator is reduced.

Circuit components II I I, l2, l8, anddtfunckg tlon exactly as described above for all light variations which occur at frequencies higher than a few per second.

For slow changes they have an additional function, that of altering the output of the generator through automatic variations of the field strength. This action will take place 'at frequencies up to alimit which is determined by the characteristics of the generator itself.

This type of circuit has practical application for such operations as the printing of motion picture film where it is imperative that the average value of light intensity be kept constant and where rapid variations of intensity or 'as little as a few per cent mayruin the print. It mayalso be utilised to compensate for variations in intensity mrmal for any carbon arc.

-In1'igure3thereisshownstcircuit whichis relerence-characters as in-Figure 1 for the purpose of convenience. In connection with Figure 3, it may be stated that this arrangement per-' mits the use of a mercury vapor lamp, which has not heretofore been possible. In the past, low

' pressure gas discharge tubes have been utilized fror modulation purposes, as for example for recording sound on but these tubes were not satisfactory 'due to lnsumcienb light intensity tion with Figure 1.

electron discharge tube l l is placed a light source and non-linear characteristics. When mercury was added to such lamps or used alone, the intensity was increased to the desired value but other difficulties arose. Used in this manner,

non-uniform characteristics were produced which were difficult or impossible to compensate.

The response was deficient in high frequencies,

distortion was high, and, in addition, the average intensity could not be controlled within sufficiently close limits to, meet modern requirements. Incandescent lamps have likewise been utilized for the purposes of recording and other uses involving modulation but were unsatisfactory since the thermal inertia of the filaments was too great for practical usage at high frequencies.

Recent developments of the high pressure mercury vapor lamp have reduced the noise level of such a lamp to a point where such lamps may be used as exciter lamps for purposes of sound recording. For these purposes, however, external modulating means have been employed since no practical means has been discovered for modulating the arc itself.

In making photographic sound records, 'it is customary to focus the light source on a narrow slit and to focus the image of the slit on the film. Unless the light source, lenses, cell, and all other parts ofthe system are very firmly fixed, vibration occurs which creates a variation in light intensity on the film which is eventually reproduced.as so-called microphonic noise. The

same result obtains if the filament of an incandescent lamp vibrates or the arc in a gas discharge tube does not remain in constant position. All of the above are disadvantages which are extremely difiicult to overcome by mechanical means. If a circuit such as that of Figure 3 is utilized and means provided to'illuminate the photo-electric cell l3 from a point between the last of the disturbing elements and the film, all disturbances, whether arising from the lamp itself or from any of the elements between the lamp and the film, will be compensated for.

In the circuit of Figure 3, current is supplied from the source ID to the electron discharge tube II in thesame manner as described in connec- In the plate circuit of the l2, between which and the photo-electric cell l3 a shutter I4 is interposed. The simple threeelement tube l6 of Figure 1 is replaced in the circuit of Figure 3, for the purpose of circuit simplification, by a multi-element tube 40, containing two control grids. The plate of this tube is connected in the circuit in the same manner as the plate of tube 15 of Figure 1. Tube 40 has a screen grid which is connected to a point between resistances M and 42, which resistances shunt the tube H and its load. One of the control grids of the tube to is adjustably connected to resistance 2|, which is identical with the resistance 2| of Figure 1. The second control grid of tube 40 is connected to the secondary of a transformer 43, the primary of which is the modulation input circuit.

, Other elements of the circuit, such as IT and I8, are identical with the corresponding elements of- Figure 1. Examination ofthis circuit will show that it likewise provides a negative or inverse optical feedback from the load of tube ll,

that is, from lamp I: to the input. In brief, a

fractional part of the output voltage here designated as p is fed back to the input of the amplifier. Black, in Patent No. 2,102,671, has shown that with an amplifier having again of u, when an is large as compared with unity. the relation of output voltage to the input voltage is proportional to and is independent of all other factors. In the case illustrated, the light intensity is proportional to since the feedback voltage, that is, the voltage developed across resistance 2|, is a function of the light intensity. It, therefore, follows that the light intensity will be proportional to the modulation voltage at all frequencies where the requirements of feedback and gain are met, and that the light intensity will be independent of all other factors, such as supply voltage changes, ageing of the lamp, mercury sputtering, etc.

Figure 3 illustrates only one of many circuits which may be employed-utilizing the advantages of optical feedback for such purposes as sound recording, signalling, and television. It will be obvious that electrical inverse feedback means arising-within the amplifier but also for defects arising between the point in the system where the feedback voltage is applied and the point where the useful work is done by the beam of light.

Figure 4 is a diagram of a circuit which may be used for facsimile reproduction. In this case,.

it is assumed that a document which has faded or yellowed is to be copied and that the copy is to be substantially black and white. Further, it

is assumed that the copy is to be made on an inexpensive diazo Itype paper, which paper is sensitive to ultra-violetlight only and that the document to be copied will not reflect the ultra-violet light to which the paper is. sensitive. In order to solve the problem assumed above, the circuit of Figure 1 is slightly modified by placing therein a second photo-electric cell 50, which cell is between the resistance 2| and the resistance 20. I

In operating this circuit for purposes as described, the document to be copied is scanned by well-known means by a spot of light which will be reflected from the scanned surface onto the photo-electric cell 50. Light from the tube I2 caused to" fall on cell l3 in the same manner as described with reference to Figure 1. a The first operating step is to determine the extremewaluesof intensity of light from lamp I2 which will be required to produce the desired ratioof dark to light areas on the copy. These two values may be designated at I1 and I2. With light reflected from the darkest area of the original onto cell 50 adjustments will be made to obtain intensity I: by the means described above, that is, by means of adjustment of resistance 2! and 6f shutter It. With light reflected from the lightest areas of the original on the cell 50 the gain of the amplifier will be adjusted by well-known means to change the intensity of light from the value I to value I1. With these adjustments made, a copy may be produced which will have any desired contrast. It is obvious that by altering connections the copy may be either a positive or negative copy of the original.

Optical feedback of the type described above in connection with the drawing may be employed effectively for projection type television receivers .since, as has been described, the light intensity may be made directly proportional to the modulating voltage. Means previously devised, such as the water call of Scophony, have been used to modulate high intensity light sources for television purposes but these means are very inefilcient and do not permit the undistorted passage herein disclosed may be embodied in other physical structures without departure from the novel subject matter thereof. I do not, therefore, desire to be limited to the disclosure as given for purposes of illustration but rather to the scope of the claims granted me.

What I claim is:

1. The method of controlling light intensity,

which comprises energizing a light source through an electron discharge tube, causing a portion of the light from said light source to fall upon a photo- -electric cell, and causing all components of the output of said photo-electric cell to control the plate current of said tube.

2. 'ljhe method of controlling light intensity,

which comprises energizing a light source through an electron discharge tube having an anode, a cathode, and a control grid, causing a portion of the light from said light source to fall upon a photo-electric cell, causing all components of the output of said cell to be impressed upon the input of an amplifier, and utilizing the output of said amplifier to control the grid voltage of said electron discharge tube. 1

3. The method of controlling light intensity,

I which comprises energizing a light source by means of electric currentsupplied over a plurality. oi paths, one of said paths including a current regulating device, permitting a portion and supplying energy thereto, and a.v photo-electric cell mounted inposition whereby light from said source shines on said cell, all components of the output current from said cell being efiective to alter the voltage on the control electrode of said tube.

6. In a device for controlling light intensity, the combination of an electron discharge tube having an anode, cathode and control grid, a light source connected in the output circuit of said electron discharge tube, a photo-electric cell in position to receive light from said light source, a

second electron discharge tube, means to apply all components of the voltage generated in said photo-electric cell to the grid of said second electron discharge tube, and meansto apply the voltage generated in said second electron discharge tube to the control grid of said first tube.

7. In a device for controlling light intensity, the combination of an electron discharge tube, having an anode, cathode and control grid, a light source connected inthe output circuit of said electron discharge tube, a photo-electric cell in position to receive light fromsaidlight source, a second electron discharge tube, means to apply the voltage generated in said photo-electric cell to the grid of said second tube, and means comprising an impedance in theplate circuit of said second tube and connected to the control electrode of said first tube whereby the change in voltage on the grid of said second tube is effective to cause a corresponding change in the opposite direction on the grid of said first tube.

8. In a device for controlling light intensity, an electron discharge tube, a generator, a light source energized jointly by said generator and through said tube, a connection from a field winding of said generator to said tube, a photoelectric cell positioned to receive light from said light source, and means controlled by said photoa electric cell for controlling the plate current of said tube, said means being effective to modify oi the light from said'light source to fall upon a portion of the light from said light source to fall upon a photo-electric cell, causing all components of the output of said photo-electric cell to regulate the current flowing through an amphfier tube, and permitting the changed current flow through said amplifier. tube to effect a change in voltage on the grid of the electron discharge tube to thereby control the energization of the light source.

5. Inc. device for controlling light intensity, in

combination, a light source, an electron discharge tube connected in circuit with said light source theoutput of said generator in accordance with the variation of plate current in said tube.

9. In a device for controlling the intensity of a: light source subject to intensity variations of less than one hundred per cent amplitude, in combination, a generator having a capacity sufiicient to supply said light source with unmodulated current, a second current source an amplifier connected to said light source to supply modulation current thereto, a photo-electric cell positioned to receive light from said light source, means under control of said photo-electric cell to control the output of said amplifier to compensate for said intensity variations occuring at high frequencies, and a connection from a field winding of said generator to said amplifier whereby the photoelectric cell controls the current flow to said winding and adjusts the generator output to compensate for low frequency variations in said light source. a h

10. In a device for controlling the intensity of a light source, the combination of an electron discharge tube having an anode, cathodeand control grid, a light source connected in the output. circuit of said electron discharge tube, a-

photo-electric cell in position to. receive light from said light source, a second electron discharge tube comprising an anode, cathode and a plurality of control electrodes, means to apply the voltage generated in said photo-electric cell to one of the control electrodes of said second tube, means to apply modulation voltages to a second control electrode of said second electron discharge tube, and means in the plate circuit of said second elecfier, with such polarity of direct current com- I ponents and such phase of alternating current tron discharge tube and connected to the control electrode of said first tube whereby the change in voltage on the control electrodes of the second tube areeflective to cause corresponding changes on the grid of said first tube.

11. In a device-tor copying and facsimile reproduetion, in combination, an amplifier, a current source; a light source energized'irom said current source through said amplifier, a light sensitive cell. positioned to :receive light from said light source, a second light sensitive cell adapted. to receive light from a document to becopied, and means under the joint control of said first and second light sensitive cells for controlling the gain of said amplifier.

12. In a device for copying and facsimile reproduction, in combination, an amplifier, a current source, a light source energized from said current source through said amplifier, a light sensitive cell positioned to receive light from said light source, a-second light sensitive cell adapted toreceive light from a document to be copied, means under the Joint control of said first and second light sensitive cells for controlling the gain of said amplifier, and means to adjust the Joint control means to vary the control of the amplifier gain tensity thereof, which comprises energizing the light source through an amplifier, providing the The method of modulating a light source and simultaneously controlling the average in-v components that the amplifier gain is reduced to the required value for all components.

14; In a system for controlling the average intensity and modulation 0! a light source, an amplifier having an ,input section and an output section, means for supplying a constant voltage and .a modulation voltage to the input. section of said amplifier, a lamp connected in the output section of said amplifier, photo-electric means for converting a portion of the light emitted by said lamp to voltage, and means for applying said voltage to said input section whereby .the gain of the amplifier is reduced.

' 15. In a light modulating system, the combination of'an electron discharge tube having an anode, a cathode, and a control grid, a light source connected in the output circuit of said electron discharge tube, a photo-electric cell in position to receive light from said light source, a

second electron discharge tube comprising an anode, a cathode, and a control grid, means to maintain a constant voltage at the cathode of. said second electron'discharge tube, means to 'impress all components or the voltage generated in said photo-electric cell on the grid of said secamplifier with excess gain over that required,

converting a portion of the light to voltage by photoelectric means,,and feeding back all components of said voltage to the input 01' said ampli-

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