US2282992A - Television receiver - Google Patents

Television receiver Download PDF

Info

Publication number
US2282992A
US2282992A US334531A US33453140A US2282992A US 2282992 A US2282992 A US 2282992A US 334531 A US334531 A US 334531A US 33453140 A US33453140 A US 33453140A US 2282992 A US2282992 A US 2282992A
Authority
US
United States
Prior art keywords
tube
voltage
television receiver
resistance
cathode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US334531A
Inventor
Deserno Peter
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Alcatel Lucent Deutschland AG
C Lorenz AG
Original Assignee
Standard Elektrik Lorenz AG
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Standard Elektrik Lorenz AG filed Critical Standard Elektrik Lorenz AG
Application granted granted Critical
Publication of US2282992A publication Critical patent/US2282992A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N5/00Details of television systems
    • H04N5/44Receiver circuitry for the reception of television signals according to analogue transmission standards
    • H04N5/57Control of contrast or brightness

Definitions

  • Television pictures should be adjusted not only as regardstheir brightness but should be adjusted also with a viewto obtaining the greatest possible sharpness of contrasts.
  • the adjustment is proper if .the black value of the mixture of picture and synchronizing signals acts to control the cathode ray tube to just dark. Withthe working point of the cathode ray tube positioned too far in the negative region the intensity of the dark details of the picture'is impaired thereby, whereas if the working point is too far in the positive region a dim picture is obtained. Proper adjustment is hence difficult especially to those not skilled in the art. It is therefore desirable to provide for means whereby the contrast effects of a picture are automatically given the best intensity.
  • This invention relates to a method for the filter chain, this filter chain segregating the synchronizing signals.
  • the filter chain which comprises a number of choke coils connected in series, may be arranged to segregate the synchronizing impulses while at the same time separating them into the well known picture change and line change impulses.
  • An arrangement particularly adapted for this purpose comprises means whereby the control voltage is caused to change the potentials of the Braun tube and-also those of its voltage source.
  • the control voltage may be taken from a con-v denser which is charged over a rectifier and a of amplitudes.
  • a means is used which has a time constant and is connected to the filter chain througha rectifier path.
  • Fig. l is a circuit diagram showing one embodiment of the invention, while Fig. 2 is a graphical representation referred to in explaining the function of 'this embodiment.
  • An electron tube R serves to rectify' the received amplified frequency mixture.
  • a tap m of a coupling resistance RK the Wehnelt cylinder- H of the Braun tube K is 'coupled to the tubeR.
  • the control voltage that corresponds to the black value arises at condenser C1.
  • This condenser is charged over a filter chain which comprises choke coils Di, T1 and T2 and condensers C2, C3, and over a dual diode I.
  • This diode here acts by means of that discharge path which in the drawing is shown to constitute the leithand half thereof.
  • the cathode of this discharge path is connected to a tap n of the resistance RK.
  • the respective voltage conditions will appear from 2.
  • the upper line represents the anode potential.
  • the voltage arising at condenser C1 corresponds to the distance A.- This voltage is conveyed to the negative'pole of a voltage source N, G for the Braun tube. Any, change in the control voltage therefore causes the potentials of the Braun tube and of its voltage means of the condensers C2, 73 are so tuned that from T1 the picture change impulses and from T2 the line change impulses are derived by a secondary coils u and 12, respectively.
  • Curve E, Fig. 2 illustrates the current con tions peculiar to the lefthand discharge path or system of the diode I.
  • the voltage between the anode thereof and earth only containsthe synchronizing impulses, the picture impulses not being contained therein. This voltage acts through coupling condenser 05 on the cathode of that discharge path or system which in the vdrawing forms the righthand half of diode I.
  • the cathode of this system is also joined through i a high ohmic resistance to the negative grounded pole of the anode voltage source.
  • the voltage As the voltage is negative with respect to earth it may serve directly for controlling the input voltage, thus enabling an automatic amplitude regulation thereof over line Q.
  • a circuit arrangement comprising 9. rectifier tube operativelyconnected to a source of amplified signals, a load comprising a resistance connecting the anode of said tube with a source of positive potential, a Braun tube, a tap on said resistance connected to the Wehnelt electrode of said tube to cause variation in the acceleration of electrons in said tube in accordance with signals across said resistance, a double diode tube, a circuit connected between a point on said resistance more negative than said tap and a cathode of said diode tube, a chain of tunedinductances comprising two transformers and a condenser shunted by a resistance connected between the anode associated with said cathode of the double diode and the positive terminal of said load resistance and a circuit connecting the cathode of said Braun tube to the more negative side of said condenser, the arrangement being such that the operating characteristics of
  • a television receiver in which the second cathode of the double diode is connected through a condenser to the anode of the first diode, and the second anode and the second cathode are shunted by a resistance and also acondenser comprising a. time constant device, the arrangement being such that the anode being negative in respect to ground provides a volume control voltage.
  • a television receiver in which the chain of tuned inductances include the primaries of two transformers, said transformers being so tuned that picture frame impulses are derived from the secondary of one and line impulses .from the. secondary of the other.

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Details Of Television Scanning (AREA)

Description

P, DEsERNo 2,282,992.
TELEVISION RECEIVER Filed May 11, 1940 Al/VE 6724/1/65 AWFWAS J INVENTOR. P5767? JESE/WVO means of intercoupled potentiometers.
Patented May '12, 1942 TELEVISION RECEIVER Peter Deserno, Berlin, Germany, assignor to C. Lorena Aktlengesellschaft, Berlin-TempelhoL- Germany, a company i Application May 11,1940, Serial No. 334,531
In Germany May 13, 1939 Claims.
automatic adjustment of the contrasts in pictures reproduced by television receivers of the kindoperating in accordance with the so-called gap synchronization method. 4
Television pictures should be adjusted not only as regardstheir brightness but should be adjusted also with a viewto obtaining the greatest possible sharpness of contrasts. The adjustment is proper if .the black value of the mixture of picture and synchronizing signals acts to control the cathode ray tube to just dark. Withthe working point of the cathode ray tube positioned too far in the negative region the intensity of the dark details of the picture'is impaired thereby, whereas if the working point is too far in the positive region a dim picture is obtained. Proper adjustment is hence difficult especially to those not skilled in the art. It is therefore desirable to provide for means whereby the contrast effects of a picture are automatically given the best intensity.
In this regard it has been proposed to employ regulating means which are mechanically coupled together and by which the received picture is given both the best contrast effects and the desired brightness. Such arrangements, however, have considerable disadvantages. In fact, these two adjustments are efiected by This requires the operative means to be balanced with respect to each other. Such balancing, however, is extremely difiicult to perform and, moreover, has to be accomplished every time the tube is replaced by another. It is disadvantageous also This invention relates to a method for the filter chain, this filter chain segregating the synchronizing signals. The filter chain, which comprises a number of choke coils connected in series, may be arranged to segregate the synchronizing impulses while at the same time separating them into the well known picture change and line change impulses.
With the aid of simple additional means it is possible also to eiiect an automatic regulation that the contrast efiects are adjusted-only in company with 'the brightness. The disadvantage resides in the fact that the adjustment of the brightness is correct only for a certain ratio of modulation to gap and that this ratio is liable to variations caused by the transmitter. These variations cannot be compensated on the receiving side.
'In order to overcome these drawbacks the invention described hereafter proposes to obtain an automatic adjustment of contrasts by means of a control voltage that corresponds to the black value of the received and rectified frequency mixture. I
An arrangement particularly adapted for this purpose comprises means whereby the control voltage is caused to change the potentials of the Braun tube and-also those of its voltage source. The control voltage may be taken from a con-v denser which is charged over a rectifier and a of amplitudes. To such end a means is used which has a time constant and is connected to the filter chain througha rectifier path.
In the drawing, Fig. l is a circuit diagram showing one embodiment of the invention, while Fig. 2 is a graphical representation referred to in explaining the function of 'this embodiment.
An electron tube R, Fig. 1, serves to rectify' the received amplified frequency mixture. Through a tap m of a coupling resistance RK the Wehnelt cylinder- H of the Braun tube K is 'coupled to the tubeR. The control voltage that corresponds to the black value arises at condenser C1. This condenser is charged over a filter chain which comprises choke coils Di, T1 and T2 and condensers C2, C3, and over a dual diode I. This diode here acts by means of that discharge path which in the drawing is shown to constitute the leithand half thereof. The cathode of this discharge path is connected to a tap n of the resistance RK.
The respective voltage conditions will appear from 2. The upper line represents the anode potential. The voltage arising at condenser C1 corresponds to the distance A.- This voltage is conveyed to the negative'pole of a voltage source N, G for the Braun tube. Any, change in the control voltage therefore causes the potentials of the Braun tube and of its voltage means of the condensers C2, 73 are so tuned that from T1 the picture change impulses and from T2 the line change impulses are derived by a secondary coils u and 12, respectively.
Curve E, Fig. 2, illustrates the current con tions peculiar to the lefthand discharge path or system of the diode I. The voltage between the anode thereof and earth only containsthe synchronizing impulses, the picture impulses not being contained therein. This voltage acts through coupling condenser 05 on the cathode of that discharge path or system which in the vdrawing forms the righthand half of diode I.
The cathode of this system is also joined through i a high ohmic resistance to the negative grounded pole of the anode voltage source.
The voltage conditions of this cathode are illustrated by curve F, Fig. 2. Over the righthand half of the diode a condenser C6 is charged to acquire a negative potential with respect to earth. Condenser Ca and resistance W constitute a means which has a certain time constant. This potential, characterized by distance B, corresponds to the black value.
As the voltage is negative with respect to earth it may serve directly for controlling the input voltage, thus enabling an automatic amplitude regulation thereof over line Q.
The novel arrangement, in which the potentials of the Braun tube and of the voltage source therefor are changed as a whole by the control voltage that corresponds to the black value, has
the advantage that the mean brightness of the approximately zero carrier amplitude, the black level in the transmitted picture represented by apredetermined percentage of the carrier amplitude, a circuit arrangement comprising 9. rectifier tube operativelyconnected to a source of amplified signals, a load comprising a resistance connecting the anode of said tube with a source of positive potential, a Braun tube, a tap on said resistance connected to the Wehnelt electrode of said tube to cause variation in the acceleration of electrons in said tube in accordance with signals across said resistance, a double diode tube, a circuit connected between a point on said resistance more negative than said tap and a cathode of said diode tube, a chain of tunedinductances comprising two transformers and a condenser shunted by a resistance connected between the anode associated with said cathode of the double diode and the positive terminal of said load resistance and a circuit connecting the cathode of said Braun tube to the more negative side of said condenser, the arrangement being such that the operating characteristics of the Braun tube are varied in accordance with the amplitude of the signals across said load resistance.
2. A television receiver according to claim 1 in which the second cathode of the double diode is connected through a condenser to the anode of the first diode, and the second anode and the second cathode are shunted by a resistance and also acondenser comprising a. time constant device, the arrangement being such that the anode being negative in respect to ground provides a volume control voltage.
3. A television receiver according to claim 1 in which the chain of tuned inductances serve as filters from which the synchronizing signal is derived. 4, A television receiver according to claim 1 in which the chain of tuned inductances include the primaries of two transformers.
5. A television receiver according to claim 1, in which the chain of tuned inductances include the primaries of two transformers, said transformers being so tuned that picture frame impulses are derived from the secondary of one and line impulses .from the. secondary of the other.
PETER I DESERNO.
US334531A 1939-05-13 1940-05-11 Television receiver Expired - Lifetime US2282992A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
DE213518X 1939-05-13

Publications (1)

Publication Number Publication Date
US2282992A true US2282992A (en) 1942-05-12

Family

ID=5813659

Family Applications (1)

Application Number Title Priority Date Filing Date
US334531A Expired - Lifetime US2282992A (en) 1939-05-13 1940-05-11 Television receiver

Country Status (4)

Country Link
US (1) US2282992A (en)
BE (1) BE438854A (en)
CH (1) CH213518A (en)
FR (1) FR868486A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2426419A (en) * 1942-12-23 1947-08-26 Du Mont Allen B Lab Inc Return trace blanking and mixing
US2745037A (en) * 1951-12-18 1956-05-08 Rca Corp Keying arrangement for single beam color tube

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2426419A (en) * 1942-12-23 1947-08-26 Du Mont Allen B Lab Inc Return trace blanking and mixing
US2745037A (en) * 1951-12-18 1956-05-08 Rca Corp Keying arrangement for single beam color tube

Also Published As

Publication number Publication date
BE438854A (en)
FR868486A (en) 1941-12-31
CH213518A (en) 1941-02-15

Similar Documents

Publication Publication Date Title
US2255484A (en) Automatic background control for television systems
US2792496A (en) Stabilized direct current setting apparatus
US2548436A (en) Television receiver background control circuit
US2227197A (en) Signaling system
US2240281A (en) Automatic background control
US2226994A (en) Amplitude filter
US2259520A (en) Television receiving apparatus
US2522967A (en) Video amplifier feeding constant black level output to cathoderay tube
US2158261A (en) Television receiver operating level control
US2265780A (en) Television receiving arrangement
US2303909A (en) Transmission of electrical signals
US2240490A (en) Television synchronizing and control system
US2276455A (en) Cathode-ray tube apparatus
US2211860A (en) Electrical wave segregation circuit
US2736769A (en) Noise cut-off synchronizing signal separator
US2282992A (en) Television receiver
US2229964A (en) Television synchronizing system
US2227001A (en) Regulation of television receivers
US2240593A (en) Television synchronizing and control system
US2215175A (en) Television synchronizing impulse separator circuit
US2240533A (en) Automatic control of television receiving systems
US2246947A (en) Automatic gain control
US2175335A (en) Television synchronizing circuits
US2236066A (en) Television apparatus
US2505367A (en) Television receiver brightness and contrast control