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US2304015A - Radio frequency transmission line - Google Patents

Radio frequency transmission line
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US2304015A
US2304015AUS400530AUS40053041AUS2304015AUS 2304015 AUS2304015 AUS 2304015AUS 400530 AUS400530 AUS 400530AUS 40053041 AUS40053041 AUS 40053041AUS 2304015 AUS2304015 AUS 2304015A
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transmission line
line
radio frequency
standing wave
transmitter
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US400530A
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Donald W Peterson
Edwin A Goldberg
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RCA Corp
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RCA Corp
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Ffa.
Ffa'. 5'.,l
n. w. PETERsoN r-:rAL
RADIO FREQUENCY TRANSMISSION LINE Filed June 30, :1941
2 Sheets-Sheet 1 VEJ 7 'fn-:Laan
will
Snventors .Donald WPeerson, Eaux/114.60 berg Dec. vl, 1942.@ Dpw. PETERSON E-r AL 2,304,015 I RADIO FREQUENCY TRANSMISSION LINE Filed June so, 1941j 2 sheets-sheet 2 I 3f 15 174 1.5 Dona Z'd 'Vl/.'Peegl' l E w/h fl Goldberg Patented Dec. l, 1942 UNITED STATES PATENT OFFICE RADIO FREQUENCY TRANSMISSION LINE Donald W. Peterson, Collingswood, and Edwin A. Goldberg, Haddon Heights, N. J., assignors to Radio Corporation of America, a corporation of Delaware Application June 30, 1941, Serial No. 400,530
16 Claims. (Cl. Z50- 17) This invention relates to radio frequencyV transmission lines, and more particularly to a protective device therefor.
Concentric transmission lines, such as are used with radio frequency transmitters, are known to be very costly, and for this reason a transmission line of as small size as possible is used. The size of such line which is selected for a given transmitter output will ordinarily be governed by the maximum standing wave voltage which occurs during short-circuit or open-circuit of the line. Under certain circumstances, as when the line becomes temporarily improperly terminated from some unforeseen or uncontrollable cause, a standing wave may occur which is greater than that existing during normal operation of the line. In such cases, a standing Wave voltage may result which exceeds the tolerable maximum andY causes breakdown of or other damage to the line. To guard against this possibility, it has been necessary to use transmission lines of greater size than that dictated by the aforementioned factors which govern selection of a suitable line, with the resultant increase in cost.
The primary objectl of our invention is to provide an improved radio frequency transmission line which will not be subject to the aforementioned disadvantages.
More particularly, it is an object of our invention to provide an improved protective device :'i
for radio frequency transmission lines which will protect such lines from damage upon the occur rence of undesirable standing waves therein.
Another object of our invention is to provide an improved protective device as aforesaid which will enable the use of transmission lines of least expense.
Still another object of our invention is to provide an improved protective device for radio frequency transmission lines which will promptly shut oi a transmitter connected thereto when the ratio of maximum to minimum standing wave voltage exceeds a predetermined value.
A further object of our invention is to provide an improved radio frequency transmission line which can be operated at higher voltages. than has been customary heretofore.
It is also an object of our invention to provide j ample, three rectiers may be used spaced from each other at distances equal to one-fourth and one-eighth the wavelength of the standing wave) 1 and connect their outputs to a normally balanced Y network. These rectiers respond to changes in line voltage at the points where they are respectively located, and a plurality of them should be used since, in certain cases, a single recti-v er, or even twov rectiers alone, will not always an improved transmission line and protective device therefor as above set forth which is vhighly efcient and reliable in use, simple in construcsee a change in line voltage. The output voltages of the rectiers will become increasingly unequal as the ratio of maximum to minimum standing wave voltage increases, and this inequality is em-n ployed to unbalance the Y network and change the bias on a triode coupled thereto, thereby causingits plate current to change The latter changeis used to operate a suitable relay the contacts of which are in the control circuit of the 1 transmitter. The arrangement is such that, upon Y creation of an undesirable standing wave, the relay operates to shut off the transmitter, thereby eliminating possibility of damage to the transmission line by that standing wave.
The novel features that We consider character-i istic of our invention are set forth with particuiy larityv the appended claims. The invention.' itself, however, both as to its organization and method of operation, as Well as additional objects and advantages thereof, will best be understood from the following description, when read in connection with the accompanying drawings in which Figures 1 and 2 are curves showing standingY waves with reference to which the principles em-V bodied in our invention are explained,
Figure 3 is a block diagram illustrating one ar rangement according to our invention, A'
Figure 4 is a wiring diagram showing the details thereof,
Figures 5 and 6 are equivalent electrical diagrams showing certain features of our invention',` particularly with reference to the modification shown in Fig. 4, and
Figure 7 is a wiring diagram of a portion of Y a standingwave 2 of the same wavelength as the wave I but of a much greater amplitude may result. As a consequence, the ratio of maximum to minimum voltage in the case of thewave 2 is much greater than in the case of the wave I. If this ratio exceeds a predetermined tolerable ratio, a condition such as arcing may result which would damage the line. If, however, a suitable protective device is provided to cut oi the supply of energy from the transmitter coupled to the line, the danger of damaging the line will be obviated.
Rectiers judiciously placed along the transmission line can be made to produce a change in potential across a resistor upon the occurrence of a predetermined standing wave. Such rectiers respond to the line voltage at the points where they are located, and the rectied voltage delivered thereby is a function of the line voltage at such points. In certain cases, however, a single rectifier, or even two rectifiers `spaced from each other along the line, might not always see a change in line voltage. For example, if the points A of Fig. 1 are considered, at which both the wave I and thewave 2 have the same voltage, it will be obvious that a change will not affect a single rectier placed at either of these points. Similarly, for some magnitude and location of standing Wave, two rectiers placed any distance d1 or d2 apart (Fig. 1) will not be affected by a change in voltage. However, if two rectiers are placed at the points A-A spaced from each other onefourth the wave length of the standing wave, and av third, rectifier is placed on either side of the other two rectiflers a distance one-eighth the wavelength of the standing wave, as at any of the points B in Fig. 2, there will always be a change in voltage across at least one of the rectiers. Such an arrangement is shown in Fig. 3 wherein therectiers 3, 5 and 'I are connected to a transmission line comprised of a pair of coaxial conductors 9 and II, therectiers 3 and 5 being spaced from each other a distance M4, where A is the wave length of the standing wave, and the rectier I being spaced from the rectier 5 a distance M8. Therectiers 3, 5 and 'I are connected to ay balanced Y network in each of the branches of which is included a resistor R2. Unbalance of this network in response to a change in the standing wave detected by oneor more of the rectiers may be availed of to operate a relay which turns off the transmitter. i
Referring to Fig. 4, we haveshcwn one arrangement or circuit employing the above principles.
Connected to the transmission line 9-II are theIrectiers 3, 5 and 1 spaced from each other as above described and enclosed within a grounded shield I3. Each of the rectifier units comprises a pair of serially connected capacitors C1 and Cz connected-across the conductors 9 and H, and a diodeV l5 the cathode II of which is connected to one side of the line, for example, the grounded conductor 9. The anode I9 of the diode I5 is, in each case, connected to` the common end of the capacitors C1 and C2. A third capacitor Ca is, in each case, also connected to the conductor 9, and a resistor R1 is connected between the capacitor C3 and the anodeV I9. The capacitor C1 can be varied'in value to make the rectier suitable forr operation at lower or higher power. The capacitor C2 is preferably connected to the inner conductor I I of the coaxial transmission line, and therefore its reactance is made high compared with the characteristic impedance of the line.A
Each of the `resistorsR1 is connected by a shieldedlead 2| to the high potential end of a separate one of the grounded resistors R2. Also connected to the point of highest potential of each of the resistors Rz is afull wave rectier 23 in series with which is a resistor R3 connected to thegrid 25 of atriode 21 in the output circuit of which is connected the winding 29 of a suitable relay.
The direct current produced by any oftherectifiers 3, 5 and 'I is approximately proportional to the impressed radio frequency voltage. If R1 is much smaller than R2 (for example, 1,000 ohms and 100,000 ohms, respectively), a maximum usable voltage will be produced across each of the resistors R2 which is approximately proportional to the radio frequency voltage of the line. Let
Ea, Eb, and Ec be the line voltages at the respective rectifier points a, b and c. If it is assumed that Ea is greater than Eb and that Eb is greater than Ec, the current through the resistor R3 results from the superposition of the currents I1 and I4 in the equivalent circuits of Figs. 5 and 6.
Let E1, E2 and Ea be the potentials across the respective resistors Rza, Rzb, and Rzc produced by the rectified currents. Y Let Rd be the resistance of eachdiode 23 where it is assumed that the resistance of each is the same. The Kirchoffs equations for Fig. 5 will then be as follows, bearing in mind that I3=I1Iz:
E1 (Rd-I-R3) I1-RdI2-E2=0 (1) Ei- (Ra-I-Rs) I1-Rd(I1-I2) -E3=0 (2) Simultaneous solution yields:
2E1- E2- E3 I1- 3Rd+2R3 (3) Kirchoffs equation for` Fig. 6 results in:
E2- E, I4-2Rd+R3 Let the potential drop across R3=Eg.
Examination of Equation 6 shows that if E1=E2=E3, then Eg=0. If E1=E2, and E3 E1, then, Eg. If E1 E1 E3,gthen,V again EgO.
Current through the resistor R3 always must be in the same direction. Therectiers 23 which will rectify both positive and negative half cycles of the currents derived from the transmission line, are arranged in. opposite relation, in pairs, to insure this result. This direction is preferablyv chose to make thegrid 25 of the triode 2.1 become 'less negative for an increase in standing wave, so.
that the relay 29 can be operated when the standing wave increases. Thisrelaymay then be madeV to open aswitch 3| in circuit Vwith the transmitter to shut 01T the transmitter, or disconnect-it from: Preferably, the relay 29" `With the above described arrangement, Acare' must be taken to keep radio frequency current outf of the D.C. circuits.- For this purpose,thecal pacitor C3 is provided which, in combination with the resistor R1, in each case, provides a path forA and filters out the radio frequency current. -It isalso for this reason that the shield I3 is provided. In operation of the device, thetriode 21 is preferably biased to a plate current lower than that required to operate the relay 29. After the transmitter is turned on, the resistor R3 is adjusted to a point where the relay will operate upon a slight increase of Eg, which opposes the bias supplied by the battery in the grid circuit. Thus, y
'the other side thereof is connected to the cathode I 'l of the rectifier l5 in each case. The anode I9 of each rectier is connected through a resistor R4 to the other transmission line conductor Il, the resistor R4 being shunted by a capacitor C5. Connection is made from each of the cathodes I1 of this modification to each of the points a, b, c of the resistors Rza, Rza, and Rza of Figure 4, respectively, the circuits being otherwise the same as above described in connection with the modification shown in Fig. 4. 'I'he conductor 3'! in this modication of the invention, which shorts 4the transmission line conductors, provides a D.-C. path for the rectified currents but appears as a very high shunt impedance at the operating frequency and therefore does not materially affect the characteristics of the line.
From the foregoing description, it will be apparent to those skilled in the art that we have provided a simple and effective way of protecting radio frequency transmission lines from becoming damaged as a result of excessive voltages resulting from undesirable standing waves. Although there are shown and described but two forms of our invention, it will be apparent to those skilled in the art that many other modifi-cations thereof are possible. 4We, therefore, desire it to be understood that we do not wish. to limit ourselves eX- cept i n so far as is made necessary by the prior art and by the spirit of the appended claims,
We claim as our invention:
1. In a system including a transmitter having a control switch in circuit therewith and coupled to a -transmission line subject to normal and abnormal standing waves, said system also including a normally balanced network coupled to said transmission line and subject to balance and unbalance depending upon whether said transmission line is subject to said normal or to said abnormal wave, respectively, and also including a grid controlled electron discharge device, the method of controlling said transmitter which comprises deriving electrical energy from said Waves at a plurality of points spaced along said waves, rectifying said energy, applying said rectified energy to said network, deriving a potential from said network when it becomes unbalanced in response to said abnormal wave, applying said potential to the control electrode of said grid controlled electron discharge device whereby to alter the output of said device, and utilizing said altered output to actuate said switch to shut oif said transmitter when said abnormal wave occurs.l
2. In a system including a transmitter having a control switch in circuit therewith and coupled to a transmission line subject to normal and abnormal standing waves, said system also including transmission line and subject to balance and unbalance depending upon whether said transmission line is subject to said normal or to said abnormal wave, respectively, and also including a grid controlled electron discharge device, the method of controlling said transmitter which comprises deriving from said waves currents at a plurality of points spaced along said waves, rectifying said currents, applying said rectified currents to said network, deriving a potential from said network when it becomes unbalanced `in response to said abnormal wave, applying said potential to the control electrode of triode said electron discharge device whereby to alter the output thereof, and utilizing said altered output to actuate said switch to shut off said transmitter when said abnormal wave occurs.
3. In a combined transmitter having a control switchin circuit therewith and a transmission line coupled thereto, said transmission line being subject to a normal standing wave during normal operation and an undesired standing wave during abnormal operation, the method of controlling said transmitter which comprises deriving current from said waves at each of a plurality of spaced points therealong, rectifying each of said currents, feeding each of said rectified currents along separate paths including a common resistor, deriving a biasing potential from said resistor, applying said biasing potential to the control electrode of a grid controlled electron discharge device whereby to alter the output of said device,
and utilizing said altered output to actuate said switch to shut off said transmitter when said undesired standing wave has reached a magnitude such that the ratio of maximum to minimum voltage resulting therefrom has exceeded a predetermined value.
4. The method set forth inclaim 3 characterized in that two of said currents are derived at points spaced along said standing waves substantially one-fourth the wavelength thereof, and .characterized further in that a third of said currents is derived at a point spaced along said waves from at least one of said first named points substantially one-eighth the wavelength thereof..
5. In a radio frequency transmitting system,
. the combination of a transmission line adapted a normally balanced Y-network coupled to said to be connected toa radio frequency transmitter and subject to a predetermined standing wave under normal operating conditions, a control circuit for sai-d transmitter including a relay, an electron discharge device including a control electrode, said relay being connected in the output 'circuit of said device, a plurality of rectiiiers connected to said line at spaced points therealong for rectifying voltages derived from said line, the spacing of said rectifers along said line being such that at least one of said rectiflers will respond to a change in voltage resulting from a change in magnitude of said standing wave produced by abnormal operating conditions, and means for applying the output of said one rectifyying device to said control electrode whereby to alter the bias thereon and thereby alter said output circuit for operating said relay. i
6. The invention set forth in claim 5 characterized in that at least three rectiflers are employed two of which are spaced from each other a distance along .said transmission line equal to substantially one-fourth the wavelength of said standing waves, and the third of which is spaced from at least one of said two rectiers a distance along said line equal to substantiallyone-eighth the wavelength of said standing waves.
7. In a radio frequency transmitting system, the combination of a transmitter including a ccntrol switch therefor, a transmission line coupled to said transmitter, said line being subject to a normal standing wave under normal operating conditions and to an undesired standing wave under abnormal operating conditions, means for deriving from either of said standing waves at a plurality of spaced points therealong a current, means for rectifying each of said currents, means providing a separate path for each of said rectified currents and including a resistor common to all of said paths, an electron discharge device having a control electrode, means for deriving a biasing potential from said resistor and applying it to said control electrode, and a relay associated with said switch, said relay being connected in the output circuit of said electron discharge device and being operable to actuate said switch upon application of a predetermined potential to said control electrode derived from said resistor in response to said undesired standing wave.
8. The invention set forth inclaim 7 characterized in that said normal standing Wave is of a magnitude such as to have a predetermined maximum to minimum voltage ratio, and characterized further in that said relay is operated when the undesired standing wave is of a magnitude such that said ratio is substantially exceeded.
9. 'I'he invention set forth inclaim 7 characterized in that said paths are connected in Y relation, chara-cterized further in that each of the branches of said Y includes a resistor, and characterized still further in that each of said resistors is connected to a separate one of said rectifying means, whereby rectified current is supplied to each of said resistors, said Y constituting .a network which is normally balanced when said transmission line is subject to said normal standing Wave, and said network becoming unbalanced when said transmission line becomes subject to an undesired standing wave to produce a current through said rst named common resistor eiective to provide the biasing potential necessary to alter the output of said electron discharge device.
10. The invention set forth in claim '7 characterized in that each of said paths includes means for rectifying both positive and negative half cycles of the currents derived from said transmission line, said last named means all bei ing connected in series with said resistor.
1v1. In a radio frequency transmission line, the combination of a pair of conductors, a pair of serially connected capacitors connected across said conductors, a rectier having a pair of cooperating electrodes, one of said electrodes being connected to one of said conductors and the other of said electrodes being connected to the common end of said capacitors, a third capacitor having one end connected to said rst named conductor, and a resistor connecting said second named electrode with the other end of said third capacitor.
.12. The invention set forth in claim l1 characterized in that one of said conductors is connected to ground, characterized further in that one of said electrodes is a cathode, and characterized still further in that said cathode is connected to said grounded conductor.
13. In a radio frequency transmission line, the combination of a pair ofconductors, a third conductor connected across said pair of conductors, and a rectifying circuit also connected across said pair of conductors in parallel relation to said third conductor, said circuit comprising a capacitor connected to one of said pair of conductors, a rectifier having a pair of electrodes one of which is connected to said capacitor, and a resistor connecting the other of said electrodes to the second one of said pair of conductors.
14. The invention set forth inclaim 13 char-V acterized in that said transmission line is subject to a standing Wave, and characterized further in that said third conductor lis of a length equal substantially to one-fourth the wave length of said standing wave.
15. The invention set forth inclaim 14 characterized by the addition of a second capacitor connected in shunt relation to said resistor.
16. The invention set forth inclaim 14 characterized in that one of said rst named pair of conductors is connected to ground, characterized further in that said capacitor is connected to said grounded conductor, characterized further in that one of said rectifier electrodes is a cathode, and
characterized still further in that said cathode is connected to said capacitor.
DONALD W. PETERSON. EDWIN A. GOLDBERG.
MME-HM 1 vvvvv A Y CERTIFICATE OF CORRECTION. Patent No. 25501;,015. K Decemberl l, 19ML DONALD W. PETERSOBLET AL.
It is hereby certified that error appears in the printed specification of the above numbered patent requiring correction aa follows: Page 5, .sec-
ond column, line l5,claim 2, strike out "triode"; page Lp, second cuolmnm: line 57', claim l5, and line MO, claim 16, for the claim reference numeral "lli" read -l5; and that the said letters Patent should be read with this 4 correction therein that the same may conform to the record of the case in the Patent Office..
signed and sealed this 11th day of December, A. D. 1915.
Leslie Frazer (Seal) First Assistant Commissioner of Patents.
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Cited By (7)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US2456800A (en)*1944-12-011948-12-21Hazeltine Research IncImpedance matching arrangement
US2498719A (en)*1947-06-071950-02-28Raytheon Mfg CoHigh-frequency protective circuits
US2498720A (en)*1947-02-061950-02-28Raytheon Mfg CoHigh-frequency protective circuits
US2575799A (en)*1948-05-271951-11-20Bell Telephone Labor IncHigh-frequency power and impedance monitor
US2579464A (en)*1946-06-181951-12-25Jr Robert John BergemannStanding wave recorder
US2605413A (en)*1943-11-101952-07-29Luis W AlvarezAntenna system with variable directional characteristic
US2837641A (en)*1953-10-011958-06-03IbmRadio frequency actuated transfer relay

Cited By (7)

* Cited by examiner, † Cited by third party
Publication numberPriority datePublication dateAssigneeTitle
US2605413A (en)*1943-11-101952-07-29Luis W AlvarezAntenna system with variable directional characteristic
US2456800A (en)*1944-12-011948-12-21Hazeltine Research IncImpedance matching arrangement
US2579464A (en)*1946-06-181951-12-25Jr Robert John BergemannStanding wave recorder
US2498720A (en)*1947-02-061950-02-28Raytheon Mfg CoHigh-frequency protective circuits
US2498719A (en)*1947-06-071950-02-28Raytheon Mfg CoHigh-frequency protective circuits
US2575799A (en)*1948-05-271951-11-20Bell Telephone Labor IncHigh-frequency power and impedance monitor
US2837641A (en)*1953-10-011958-06-03IbmRadio frequency actuated transfer relay

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