DE620173C - Device to compensate for image distortions in television cathode ray tubes - Google Patents

Device to compensate for image distortions in television cathode ray tubes

Info

Publication number
DE620173C
DE620173C DER89071D DER0089071D DE620173C DE 620173 C DE620173 C DE 620173C DE R89071 D DER89071 D DE R89071D DE R0089071 D DER0089071 D DE R0089071D DE 620173 C DE620173 C DE 620173C
Authority
DE
Germany
Prior art keywords
cathode ray
compensate
ray tubes
image distortions
screen
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
Application number
DER89071D
Other languages
German (de)
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.)
RCA Corp
Original Assignee
RCA Corp
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.)
Publication date
Priority to DER89071D priority Critical patent/DE620173C/en
Priority claimed from US640169A external-priority patent/US1995376A/en
Application granted granted Critical
Publication of DE620173C publication Critical patent/DE620173C/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/70Arrangements for deflecting ray or beam
    • H01J29/72Arrangements for deflecting ray or beam along one straight line or along two perpendicular straight lines
    • H01J29/76Deflecting by magnetic fields only

Landscapes

  • Transforming Electric Information Into Light Information (AREA)
  • Details Of Television Scanning (AREA)

Description

Einrichtung zum Ausgleich von Bildverzerrungen bei Fernsehkathodenstrahlröhren Bei der Verwendung von Kathodenstrahlröhren zur Bildzerlegung auf der Senderseite wird in der Regel ein photoaktiver Schirm benutzt, der zur Achse des Elektrodensystems geneigt angeordnet ist. Bei einer solchen Anordnung hat aber das auf dem Schirm abgetastete Bildfeld keine rechteckige, sondern eine trapezförmige Gestalt. Die vorliegende Erfindung gibt nun ein Mittel an; um diese Verzerrung auszugleichen.Device to compensate for image distortions in television cathode ray tubes When using cathode ray tubes for image decomposition on the transmitter side Usually a photoactive screen is used, which is the axis of the electrode system is arranged inclined. With such an arrangement, however, that has on the screen The scanned image field is not a rectangular, but a trapezoidal shape. the The present invention now provides a means; to compensate for this distortion.

In der Zeichnung zeigen die Abb. i und 2 (Schnitt nach 2-2 in Abb. i) Teile eines Kathodenstrahlfernsehsenders. io ist die Abtaströhre mit dem photoaktiven Schirm 12, 14, auf den das Bild des beweglichen Films 16 durch die Optik 17 geworfen wird, deren Achse 18 senkrecht zur Fläche des Schirmes steht. 2o ist die Elektronenquelle, 22 die Achse des Kathodenstrahls, der etwa 6o° zu der Schirmfläche geneigt ist; 28 sind die waagerechten Ablenkspulen (Frequenz 24 Hz) und 32 die vertikalen Ablenkspulen (432o Hz). Die Projektion des Bildes auf den Schirm 14 hat die Aufspeicherung kleiner elektrostatischer Ladungen auf der Schirmfläche zur Folge; jede Ladung ist proportional dem entsprechenden Helligkeitswert. Wenn der Strahl 24 den Schirm 1q. abtastet, werden diese Ladungen neutralisiert und entwickeln die zu übertragenden elektrischen Werte. .In the drawing, Figs. I and 2 (section according to 2-2 in Fig. i) Parts of a cathode ray television transmitter. io is the scanning tube with the photoactive one Screen 12, 14 onto which the image of the moving film 16 is thrown by the optics 17 whose axis 18 is perpendicular to the surface of the screen. 2o is the electron source, 22 the axis of the cathode ray, which is inclined about 60 ° to the screen surface; 28 are the horizontal deflection coils (frequency 24 Hz) and 32 are the vertical deflection coils (432o Hz). The projection of the image on the screen 14 has the accumulation smaller electrostatic charges on the screen surface result; every charge is proportional the corresponding brightness value. When the beam 24 passes the screen 1q. scans, these charges are neutralized and develop the electrical ones to be transferred Values. .

Bei dem dargestellten System würde der Strahl 24 auf dem Schirm 14 über eine trapezförmige FlächeA-B-C-D (Abh.3) abtasten; diese Fläche würde dann an der Empfangsstelle die Wiedergabe eines verzerrten Bildes zur Folge haben.In the illustrated system, the beam 24 would be on the screen 14 scan over a trapezoidal surface A-B-C-D (Fig. 3); this area would then result in the reproduction of a distorted picture at the receiving station.

Zum Ausgleich dieser Verzerrung wird einzusätzliches festes magnetisches Feld vorgesehen, dessen Kraftlinien so verteilt und gerichtet sind, daß der Strahl in der senkrecht zur Achse 22 verlaufenden Ebene eine umgekehrt trapezförmige Fläche E-F-G-H (Abb. 3) abtasten würde, wenn es nur allein vorhanden wäre. Die Summenwirkung mit dein von den Ablenkspulen erzeugten Felde ist dann die, daß auf dein Schirm 14 eine rechtwinklige Fläche abgetastet wird.To compensate for this distortion, an additional solid magnetic Field provided, the lines of force are so distributed and directed that the beam an inverted trapezoidal surface in the plane perpendicular to the axis 22 E-F-G-H (Fig. 3) would scan if it were only there. The cumulative effect the field generated by the deflection coils is then that on your screen 14 a rectangular surface is scanned.

Das feste magnetische Feld wird durch einen Hufeisenmagneten 34 hervorgerufen, dessen Pole 36 und 38 auf den beiden Seiten der Röhrenachse 22 liegen, nach dein Schirm 14 hin gerichtet sind und sich etwas über die Ablenkspulen hinaus erstrecken, so daß der Strahl24 zuerst durch das sich konstant ändernde Ablenkfeld der Magnetspulen und dann durch das feste Trapezkorrektionsfeldhindurchgeht. Die Pole 36 und 38 liegen ferner symmetrisch zur Achse 40, welche die Achse 22 senkrecht schneidet. Die Achse 42 des Magneten 34 verläuft parallel zur Achse 22 und liegt in der durch 22 und 4o bestimmten Ebene. An Stelle des Dauermagneten 34 kann auch ein Elektromagnet verwendet werden, der den Vorteil leichter Einstellbarkeit bietet. Wenn die Fläche T-K-L-111, die der Strahl abtastet, etwa noch verzerrte Ecken aufweist, wie durch die punktierten Linien in Abb.4 angedeutet ist, kann diese Verzerrung durch Hilfsmagnete 44 korrigiert werden, die in der aus Abb. i und 2 ersichtlichen Weise zu beiden Seiten der Achse 22 angeordnet sind.The fixed magnetic field is created by a horseshoe magnet 34, whose poles 36 and 38 lie on the two sides of the tube axis 22, according to your Screen 14 are directed towards and extend somewhat beyond the deflection coils, so that the beam 24 first through the constantly changing deflection field of the magnet coils and then passes through the fixed keystone correction field. Poles 36 and 38 are located furthermore symmetrical to the axis 40, which intersects the axis 22 perpendicularly. The axis 42 of the magnet 34 runs parallel to the axis 22 and lies in the through 22 and 4o specific level. Instead of the permanent magnet 34, an electromagnet can also be used be used, which offers the advantage of easy adjustability. When the area T-K-L-111, which the beam scans, still has distorted corners, such as through the dotted lines indicated in Fig.4, this distortion can be caused by auxiliary magnets 44 must be corrected, as can be seen from Figs. I and 2 for both Sides of the axis 22 are arranged.

Claims (2)

PATENTANSPRÜCHE i. Einrichtung zum Ausgleich von Bildverzerrungen bei Fernsehkathodenstrahlröhren, dadurch gekennzeichnet, daß -ein von der Wirkung der Ablenkspulen unabhängiges zusätzliches Magnetfeld vorgesehen ist. PATENT CLAIMS i. Device for compensating for image distortions in television cathode ray tubes, characterized in that an additional magnetic field independent of the action of the deflection coils is provided. 2. Einrichtung nach Anspruch i, dadurch gekennzeichnet, daß das zusätzliche Magnetfeld von einem Hufeisenmagneten hervorgerufen wird, dessen Pole parallel zur Röhrenachse und in gleichem Abstand von ihr angeordnet sind.2. Establishment according to claim i, characterized in that the additional magnetic field of one Horseshoe magnet, the poles of which are parallel to the tube axis and in are arranged at the same distance from it.
DER89071D 1932-10-29 Device to compensate for image distortions in television cathode ray tubes Expired DE620173C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
DER89071D DE620173C (en) 1932-10-29 Device to compensate for image distortions in television cathode ray tubes

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DER89071D DE620173C (en) 1932-10-29 Device to compensate for image distortions in television cathode ray tubes
US640169A US1995376A (en) 1932-10-29 1932-10-29 Television system

Publications (1)

Publication Number Publication Date
DE620173C true DE620173C (en) 1935-10-15

Family

ID=25992444

Family Applications (1)

Application Number Title Priority Date Filing Date
DER89071D Expired DE620173C (en) 1932-10-29 Device to compensate for image distortions in television cathode ray tubes

Country Status (1)

Country Link
DE (1) DE620173C (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE923805C (en) * 1951-04-28 1955-02-21 Telefunken Gmbh Arrangement for magnetic beam deflection in cathode ray tubes
DE972332C (en) * 1938-11-24 1959-07-02 Fernseh Gmbh Electromagnetic deflection device for cathode ray tubes, especially for televisions
DE1111302B (en) * 1958-09-10 1961-07-20 Telefunken Patent Arrangement for linearizing the written grid of a cathode ray tube
DE1157711B (en) * 1961-12-01 1963-11-21 Nordmende Device for correcting the geometry of television images

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE972332C (en) * 1938-11-24 1959-07-02 Fernseh Gmbh Electromagnetic deflection device for cathode ray tubes, especially for televisions
DE923805C (en) * 1951-04-28 1955-02-21 Telefunken Gmbh Arrangement for magnetic beam deflection in cathode ray tubes
DE1111302B (en) * 1958-09-10 1961-07-20 Telefunken Patent Arrangement for linearizing the written grid of a cathode ray tube
DE1157711B (en) * 1961-12-01 1963-11-21 Nordmende Device for correcting the geometry of television images

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