DE583864C - Circuit for receiving modulated high-frequency waves - Google Patents
Circuit for receiving modulated high-frequency wavesInfo
- Publication number
- DE583864C DE583864C DET39009D DET0039009D DE583864C DE 583864 C DE583864 C DE 583864C DE T39009 D DET39009 D DE T39009D DE T0039009 D DET0039009 D DE T0039009D DE 583864 C DE583864 C DE 583864C
- Authority
- DE
- Germany
- Prior art keywords
- circuit
- tube
- frequency waves
- receiving modulated
- rectifier
- 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
Links
- 239000003990 capacitor Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000000903 blocking effect Effects 0.000 description 1
- 230000008030 elimination Effects 0.000 description 1
- 238000003379 elimination reaction Methods 0.000 description 1
- 238000005562 fading Methods 0.000 description 1
- 238000012886 linear function Methods 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03D—DEMODULATION OR TRANSFERENCE OF MODULATION FROM ONE CARRIER TO ANOTHER
- H03D1/00—Demodulation of amplitude-modulated oscillations
- H03D1/14—Demodulation of amplitude-modulated oscillations by means of non-linear elements having more than two poles
- H03D1/16—Demodulation of amplitude-modulated oscillations by means of non-linear elements having more than two poles of discharge tubes
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03G—CONTROL OF AMPLIFICATION
- H03G3/00—Gain control in amplifiers or frequency changers
- H03G3/20—Automatic control
- H03G3/22—Automatic control in amplifiers having discharge tubes
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B14/00—Transmission systems not characterised by the medium used for transmission
- H04B14/002—Transmission systems not characterised by the medium used for transmission characterised by the use of a carrier modulation
- H04B14/004—Amplitude modulation
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Amplifiers (AREA)
- Circuits Of Receivers In General (AREA)
- Control Of Amplification And Gain Control (AREA)
- Mobile Radio Communication Systems (AREA)
- Transmitters (AREA)
- Rectifiers (AREA)
- Hybrid Cells (AREA)
- Noise Elimination (AREA)
Description
DEUTSCHES REICHGERMAN EMPIRE
AUSGEGEBEN AM
11. SEPTEMBER 1933ISSUED ON
SEPTEMBER 11, 1933
REICHSPATENTAMTREICH PATENT OFFICE
PATENTSCHRIFTPATENT LETTERING
JVl 583864 KLASSE 21a4 GRUPPE 29JVl 583864 CLASS 21a 4 GROUP 29
T3900P VIIIaJ2iai Tag der Bekanntmachung über die Erteilung des Patents:T3900P VIIIaJ2ia i Date of the announcement of the grant of the patent: 19331933
Schaltung zum Empfang modulierter hochfrequenter WellenCircuit for receiving modulated high-frequency waves
Zusatz zum Patent 580991Addition to patent 580991
Patentiert im Deutschen Reiche vom 18. Juni 1931 ab Das Hauptpatent hat angefangen am 7. Juni 1931.Patented in the German Empire on June 18, 1931 The main patent started on June 7, 1931.
Im Patent 580 991 ist eine Gleichrichterschaltung beschrieben, die die Behebung der Fadings beim Empfang ermöglicht, indem Anwendung einer stetig wirkenden Gleichrichterstufe mit logarithmischer Gleichrichtkennlinie vorgesehen ist.In the patent 580 991 a rectifier circuit is described which the elimination of the Fadings during reception are made possible by using a continuously acting rectifier stage is provided with a logarithmic rectification characteristic.
Gemäß der vorliegenden Erfindung findet als Gleichrichterstufe die Kombination eines beliebigen Gleichrichters und eines entsprechend verzerrenden Verstärkers Anwendung. According to the present invention, the combination of a rectifier stage any rectifier and a correspondingly distorting amplifier application.
Es sei E die Feldstärke eines ankommenden unmodulierten Zeichens, und der durch die Gleichrichtung erhaltene Gleichstrom sei gegeben durch die Gleichrichtkennlinie, die der GleichungLet E be the field strength of an incoming unmodulated character, and let the direct current obtained by the rectification be given by the rectification characteristic, that of the equation
Jg = ψ (E)J g = ψ (E)
genügt. Die Kennlinie des Verstärkers für die gleichgerichteten Schwingungen sei weitergegeben durchenough. The characteristic of the amplifier for the rectified vibrations is passed on by
jv==f(Jt)=f(?pE),j v == f (J t ) = f ( ? p E),
wo /„ die verstärkte Stromstärke ist.where / "is the amplified amperage.
Es ist nun möglich, die Funktionen ψ und / so zu wählen, daß diese letzte Gleichung den Charakter annimmtIt is now possible to choose the functions ψ and / in such a way that this last equation takes on the character
Jg = log nat E -\- Konstanz. J g = log nat E - \ - constancy.
An sich ist diese Bedingung auf unendlich viele Arten zu erfüllen.In itself, this condition can be met in an infinite number of ways.
Als einfaches Beispiel sei der Fall dargestellt, daß die Gleichrichtkennlinie "eine lineare ist, während die Verstärkung einem logarithmischen Gesetz folgt:As a simple example, the case is shown that the rectification characteristic "a is linear, while the gain follows a logarithmic law:
JV=B log nat JS=B log nat E-\-B log nat A. J V = B log nat J S = B log nat E - \ - B log nat A.
Diese Lösung führt zu einer technisch einfachen Ausführung, deren Prinzip in der Abbildung dargestellt ist. Hierin ist 1 das Gleichrichtrohr, in dem die Gleichrichtung durch das bekannte Audionprinzip mittels des Blockkondensators 2 und des Widerstandes 3 über einen möglichst großen Bereich linear gemacht ist. Der mittlere Wert der Gitterspannung der Röhre 1 und infolgedessen auch der mittlere Wert des SpannungsabfallesThis solution leads to a technically simple design, the principle of which in the Figure is shown. Here 1 is the rectifier tube in which the rectification by the well-known audion principle by means of the blocking capacitor 2 and the resistor 3 is made linear over as large a range as possible. The mean value of the grid voltage of the tube 1 and consequently also the mean value of the voltage drop
*) Von dem Patentsucher ist als der Erfinder angegeben worden:*) The patent seeker stated as the inventor:
Dr. Hans-Otto Roosenstein in Berlin.Dr. Hans-Otto Roosenstein in Berlin.
auf dem Widerstand 4 sind also lineare Funktionen der Feldstärke des ankommenden Zeichens. Der Kondensators dient als Kurzschluß für die Hochfrequenzwechselspannung. Die ganze gleichgerichtete Stromstärke, d. h. ihr Niederfrequenzanteil und ihr Gleichstromanteil zusammen, ist über den extrem hohen Widerstand 6 (z.B. 100 Megohm) an das Gitter der Verstärkerröhre 7 geto legt. Die Verstärkerröhre arbeitet im Gebiet negativer Gitterspannung, in dem bekanntlich für große Bereiche des Gitterstromes ig das Gesetz gilt:on the resistor 4 there are therefore linear functions of the field strength of the incoming character. The capacitor serves as a short circuit for the high-frequency AC voltage. The entire rectified current intensity, ie its low frequency component and its direct current component together, is passed to the grid of the amplifier tube 7 via the extremely high resistance 6 (eg 100 megohms). The amplifier tube works in the area of negative grid voltage, in which, as is well known, the law applies to large areas of the grid current i g:
ig=. A- eBv3 (1)i g =. A- e Bv 3 (1)
(e = Basis nat log System, vg = Gitterspannung, A und B sind Konstanten). Der Widerstand S habe einen so großen Wert R, daß er praktisch allein bestimmend für die Stromstärke ig ist. Weiter sei der Abzweig F so einreguliert, daß zwischen den Punkten E und F kein Gleichspannungsunterschied besteht, wenn kein Signal auf den Empfänger auftrifft. Ein Signal verursache eine Spannungserhöhung ν von E gegenüber F,. und der verursachte Gitterstrom berechnet sich nach dem Vorhergesagten angenähert zu (e = basis nat log system, v g = grid voltage, A and B are constants). The resistance S has such a large value R that it is practically the sole determinant of the current i g . Furthermore, the branch F is adjusted so that there is no DC voltage difference between points E and F when no signal is incident on the receiver. A signal causes a voltage increase ν of E compared to F ,. and the grid current caused is calculated according to the predicted approximately to
(2)(2)
(2) in (1) ergibt(2) in (1) results
log nat ν = B vs + log nat A R. log nat ν = B v s + log nat A R.
In Worten besagt diese Gleichung, daß die Gitterspannung der Verstärkerröhre die gewünschte logarithmische Funktion der gleichgerichteten Spannung und damit der ankommenden Hochfrequenzfeldstärke ist.In words this equation says that the grid voltage of the amplifier tube is the desired logarithmic function of the rectified voltage and thus the incoming High frequency field strength is.
Daß es für die Zwecke der Erfindung nicht notwendig ist, daß der Gleichrichter linear arbeitet, wurde oben schon erwähnt, beispielsweise kann man auch mit einem rein quadratisch arbeitenden Gleichrichter denselben Effekt erzielen, muß dann aber die Verstärkerwirkung nach dem GesetzeThat it is not necessary for the purposes of the invention that the rectifier is linear works, has already been mentioned above, for example you can also use a rectifier that works purely as a square To achieve an effect, however, the reinforcing effect must then according to the law
geschehen lassen. Dieses läßt sich beispielsweise durch die Kombination der Wirkung mehrerer Röhren erreichen.let it happen. This can be done, for example, by combining the effects multiple tubes.
Claims (3)
Priority Applications (11)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DET38879D DE560227C (en) | 1931-05-18 | 1931-05-18 | Method for transmitting messages by means of high frequency waves |
DET38969D DE580991C (en) | 1931-05-18 | 1931-06-06 | Circuit for receiving modulated high-frequency waves |
DET39009D DE583864C (en) | 1931-05-18 | 1931-06-17 | Circuit for receiving modulated high-frequency waves |
FR730942D FR730942A (en) | 1931-05-18 | 1932-02-03 | Method of communication by means of high frequency waves |
DET40186D DE618797C (en) | 1931-05-18 | 1932-02-08 | Circuit for receiving modulated high-frequency waves |
US609421A US2031072A (en) | 1931-05-18 | 1932-05-05 | Method of and means for signaling |
US615647A US2014509A (en) | 1931-05-18 | 1932-06-06 | Radioreceiver |
GB15956/32A GB393415A (en) | 1931-05-18 | 1932-06-06 | Improvements in or relating to receivers for modulated high frequency waves |
GB17221/32A GB393421A (en) | 1931-05-18 | 1932-06-17 | Improvements in or relating to receivers for modulated high frequency waves |
FR43009D FR43009E (en) | 1931-05-18 | 1933-02-07 | Method of communication by means of high frequency waves |
GB3903/33A GB413402A (en) | 1931-05-18 | 1933-02-08 | Improvements in or relating to modulated carrier wave receivers |
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DET38879D DE560227C (en) | 1931-05-18 | 1931-05-18 | Method for transmitting messages by means of high frequency waves |
DET38969D DE580991C (en) | 1931-05-18 | 1931-06-06 | Circuit for receiving modulated high-frequency waves |
DET39009D DE583864C (en) | 1931-05-18 | 1931-06-17 | Circuit for receiving modulated high-frequency waves |
DET40186D DE618797C (en) | 1931-05-18 | 1932-02-08 | Circuit for receiving modulated high-frequency waves |
Publications (1)
Publication Number | Publication Date |
---|---|
DE583864C true DE583864C (en) | 1933-09-11 |
Family
ID=32034272
Family Applications (4)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
DET38879D Expired DE560227C (en) | 1931-05-18 | 1931-05-18 | Method for transmitting messages by means of high frequency waves |
DET38969D Expired DE580991C (en) | 1931-05-18 | 1931-06-06 | Circuit for receiving modulated high-frequency waves |
DET39009D Expired DE583864C (en) | 1931-05-18 | 1931-06-17 | Circuit for receiving modulated high-frequency waves |
DET40186D Expired DE618797C (en) | 1931-05-18 | 1932-02-08 | Circuit for receiving modulated high-frequency waves |
Family Applications Before (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
DET38879D Expired DE560227C (en) | 1931-05-18 | 1931-05-18 | Method for transmitting messages by means of high frequency waves |
DET38969D Expired DE580991C (en) | 1931-05-18 | 1931-06-06 | Circuit for receiving modulated high-frequency waves |
Family Applications After (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
DET40186D Expired DE618797C (en) | 1931-05-18 | 1932-02-08 | Circuit for receiving modulated high-frequency waves |
Country Status (4)
Country | Link |
---|---|
US (2) | US2031072A (en) |
DE (4) | DE560227C (en) |
FR (2) | FR730942A (en) |
GB (3) | GB393415A (en) |
Families Citing this family (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE758211C (en) * | 1937-02-11 | 1953-02-09 | Radio Transmission Equipment L | Device for displaying the deviation of a vehicle from a course line |
US2515187A (en) * | 1942-04-09 | 1950-07-18 | William R Bliss | Wide dynamic range amplifying and demodulating system |
US2577506A (en) * | 1945-07-09 | 1951-12-04 | Logan M Belleville | Amplifier |
US2662978A (en) * | 1945-11-29 | 1953-12-15 | Philco Corp | Logarithmic transducer |
US2548913A (en) * | 1946-04-17 | 1951-04-17 | Edmund D Schreiner | Radio receiver with logarithmic response circuit |
US2705794A (en) * | 1946-06-11 | 1955-04-05 | Philco Corp | Signal modifying apparatus for eliminating variations as a function of one or more independent variables |
US2663015A (en) * | 1946-06-11 | 1953-12-15 | Philco Corp | Object location system employing logarithmic transducer |
US2713162A (en) * | 1950-12-14 | 1955-07-12 | Rca Corp | Pulse receiver with logarithmic amplifier and base clipping detector |
US2823303A (en) * | 1953-10-29 | 1958-02-11 | Hoffman Electronics Corp | Compressor circuits for panoramic receivers |
DE962271C (en) * | 1954-11-12 | 1957-04-18 | Lorenz C Ag | Circuit arrangement for frequency modulation |
NL111923C (en) * | 1956-04-11 | |||
GB933934A (en) * | 1960-12-08 | 1963-08-14 | Marconi Wireless Telegraph Co | Improvements in or relating to frequency varying circuit arrangements |
-
1931
- 1931-05-18 DE DET38879D patent/DE560227C/en not_active Expired
- 1931-06-06 DE DET38969D patent/DE580991C/en not_active Expired
- 1931-06-17 DE DET39009D patent/DE583864C/en not_active Expired
-
1932
- 1932-02-03 FR FR730942D patent/FR730942A/en not_active Expired
- 1932-02-08 DE DET40186D patent/DE618797C/en not_active Expired
- 1932-05-05 US US609421A patent/US2031072A/en not_active Expired - Lifetime
- 1932-06-06 US US615647A patent/US2014509A/en not_active Expired - Lifetime
- 1932-06-06 GB GB15956/32A patent/GB393415A/en not_active Expired
- 1932-06-17 GB GB17221/32A patent/GB393421A/en not_active Expired
-
1933
- 1933-02-07 FR FR43009D patent/FR43009E/en not_active Expired
- 1933-02-08 GB GB3903/33A patent/GB413402A/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
US2031072A (en) | 1936-02-18 |
DE618797C (en) | 1935-09-17 |
FR43009E (en) | 1934-01-25 |
GB393421A (en) | 1933-06-08 |
US2014509A (en) | 1935-09-17 |
DE580991C (en) | 1933-07-19 |
GB393415A (en) | 1933-06-08 |
GB413402A (en) | 1934-07-19 |
FR730942A (en) | 1932-08-26 |
DE560227C (en) | 1932-09-29 |
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