Army Radio Communication in the Great War Keith R Thrower, OBE
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Toward a Large Bandwidth Photonic Correlator for Infrared Heterodyne Interferometry a first Laboratory Proof of Concept
A&A 639, A53 (2020) Astronomy https://doi.org/10.1051/0004-6361/201937368 & c G. Bourdarot et al. 2020 Astrophysics Toward a large bandwidth photonic correlator for infrared heterodyne interferometry A first laboratory proof of concept G. Bourdarot1,2, H. Guillet de Chatellus2, and J-P. Berger1 1 Univ. Grenoble Alpes, CNRS, IPAG, 38000 Grenoble, France e-mail: [email protected] 2 Univ. Grenoble Alpes, CNRS, LIPHY, 38000 Grenoble, France Received 19 December 2019 / Accepted 17 May 2020 ABSTRACT Context. Infrared heterodyne interferometry has been proposed as a practical alternative for recombining a large number of telescopes over kilometric baselines in the mid-infrared. However, the current limited correlation capacities impose strong restrictions on the sen- sitivity of this appealing technique. Aims. In this paper, we propose to address the problem of transport and correlation of wide-bandwidth signals over kilometric dis- tances by introducing photonic processing in infrared heterodyne interferometry. Methods. We describe the architecture of a photonic double-sideband correlator for two telescopes, along with the experimental demonstration of this concept on a proof-of-principle test bed. Results. We demonstrate the a posteriori correlation of two infrared signals previously generated on a two-telescope simulator in a double-sideband photonic correlator. A degradation of the signal-to-noise ratio of 13%, equivalent to a noise factor NF = 1:15, is obtained through the correlator, and the temporal coherence properties of our input signals are retrieved from these measurements. Conclusions. Our results demonstrate that photonic processing can be used to correlate heterodyne signals with a potentially large increase of detection bandwidth. -
Electret Microphone Replacement for a Carbon Insert
The VMARS Newsletter Issue 29 Electret microphone replacement for a carbon insert Colin Guy G4DDI When I found that I had a dud carbon insert in an H33F/PT handset, and I couldn’t find another insert that fitted (the original is about 1” diameter) I looked around for an alternative. Trevor Sanderson’s excellent article “The RAF Microphone” (Radio Bygones issue 79/80) makes reference to the use of electret inserts with an IC preamplifier in telephones and aircraft headsets, but the information given was too scant to make construction of one of these possible without reference to the IC data sheet, and the IC’s are expensive and difficult to obtain. I had a GPO type 21A insert, but the innards of this when dismantled were still too large to fit into the available space. The H33 handset is very slim, and also virtually solid, so there is very little room in which to place a preamplifier. A dig around on the internet turned up the following article written by F. Hueber, originally published in Elektor Electronics December 1994, and is published here with permission from Elektor Electronics magazine, December 1994, copyright Segment B.V., Beek (Lb.), The Netherlands, www.segment.nl. The original article included a pcb layout, but I built mine on a strip of veroboard four tracks wide by about 2” (see photo) and mounted it on the back of the ptt switch. The electret insert was acquired from a scrap telephone and all the rest of the components from TV panels. To save space the rectifier and R12 weren’t included, care being taken to ensure that the polarity was correct. -
Lecture 25 Demodulation and the Superheterodyne Receiver EE445-10
EE447 Lecture 6 Lecture 25 Demodulation and the Superheterodyne Receiver EE445-10 HW7;5-4,5-7,5-13a-d,5-23,5-31 Due next Monday, 29th 1 Figure 4–29 Superheterodyne receiver. m(t) 2 Couch, Digital and Analog Communication Systems, Seventh Edition ©2007 Pearson Education, Inc. All rights reserved. 0-13-142492-0 1 EE447 Lecture 6 Synchronous Demodulation s(t) LPF m(t) 2Cos(2πfct) •Only method for DSB-SC, USB-SC, LSB-SC •AM with carrier •Envelope Detection – Input SNR >~10 dB required •Synchronous Detection – (no threshold effect) •Note the 2 on the LO normalizes the output amplitude 3 Figure 4–24 PLL used for coherent detection of AM. 4 Couch, Digital and Analog Communication Systems, Seventh Edition ©2007 Pearson Education, Inc. All rights reserved. 0-13-142492-0 2 EE447 Lecture 6 Envelope Detector C • Ac • (1+ a • m(t)) Where C is a constant C • Ac • a • m(t)) 5 Envelope Detector Distortion Hi Frequency m(t) Slope overload IF Frequency Present in Output signal 6 3 EE447 Lecture 6 Superheterodyne Receiver EE445-09 7 8 4 EE447 Lecture 6 9 Super-Heterodyne AM Receiver 10 5 EE447 Lecture 6 Super-Heterodyne AM Receiver 11 RF Filter • Provides Image Rejection fimage=fLO+fif • Reduces amplitude of interfering signals far from the carrier frequency • Reduces the amount of LO signal that radiates from the Antenna stop 2/22 12 6 EE447 Lecture 6 Figure 4–30 Spectra of signals and transfer function of an RF amplifier in a superheterodyne receiver. 13 Couch, Digital and Analog Communication Systems, Seventh Edition ©2007 Pearson Education, Inc. -
HP 423A Crystal Detector
Errata Title & Document Type: 423A and 8470A Crystal Detector Operating and Service Manual Manual Part Number: 00423-90001 Revision Date: July 1976 About this Manual We’ve added this manual to the Agilent website in an effort to help you support your product. This manual provides the best information we could find. It may be incomplete or contain dated information, and the scan quality may not be ideal. If we find a better copy in the future, we will add it to the Agilent website. HP References in this Manual This manual may contain references to HP or Hewlett-Packard. Please note that Hewlett- Packard's former test and measurement, life sciences, and chemical analysis businesses are now part of Agilent Technologies. The HP XXXX referred to in this document is now the Agilent XXXX. For example, model number HP8648A is now model number Agilent 8648A. We have made no changes to this manual copy. Support for Your Product Agilent no longer sells or supports this product. You will find any other available product information on the Agilent Test & Measurement website: www.agilent.com Search for the model number of this product, and the resulting product page will guide you to any available information. Our service centers may be able to perform calibration if no repair parts are needed, but no other support from Agilent is available. OPERATING AND SERVICE MANUAL - I 423A 8470A CRYSTAL DETECTOR HEWLETT~PACKARD Plint.d: JUtY 191& e H.",len Packard Co. \910 1 " • .' • I .... ,. ", - \, . '. ~ ~.. ". ." , .' " . ..... " 'I. "",:,. • ' Page 2 i\lodel ·123A/8470A 1. GENERAL INFORMATION 10. -
Design Considerations for Optical Heterodyne
DESIGNCONSIDERATIONS FOR OPTICAL HETERODYNERECEIVERS: A RFXIEW John J. Degnan Instrument Electro-optics Branch NASA GoddardSpace Flight Center Greenbelt,Maryland 20771 ABSTRACT By its verynature, an optical heterodyne receiver is both a receiver and anantenna. Certain fundamental antenna properties ofheterodyne receivers are describedwhich set theoretical limits on the receiver sensitivity for the detectionof coherent point sources, scattered light, and thermal radiation. In order to approachthese limiting sensitivities, the geometry of the optical antenna-heterodyne receiver configurationmust be carefully tailored to the intendedapplication. The geometric factors which affect system sensitivity includethe local osciliator (LO) amplitudedistribution, mismatches between the signaland LO phasefronts,central obscurations of the optical antenna, and nonuniformmixer quantum efficiencies. The current state of knowledge in this area, which rests heavilyon modern concepts of partial coherence, is reviewed. Following a discussion of noiseprocesses in the heterodyne receiver and the manner in which sensitivity is increasedthrough time integration of the detectedsignal, we derivean expression for the mean squaresignal current obtained by mixing a coherent local oscillator with a partially coherent, quasi- monochromaticsource. We thendemonstrate the manner in which the IF signal calculationcan be transferred to anyconvenient plane in the optical front end ofthe receiver. Using these techniques, we obtain a relativelysimple equation forthe coherently detected signal from anextended incoherent source and apply it to theheterodyne detection of an extended thermal source and to theback- scatter lidar problem where the antenna patternsof both the transmitter beam andheterodyne receiver mustbe taken into account. Finally, we considerthe detectionof a coherentsource and, in particular, a distantpoint source such as a star or laser transmitter in a longrange heterodyne communications system. -
Crystal Receivers for Broadcast Reception
CRYSTAL RECEIVERS FOR BROADCAST RECEPTION BY PERCY W. HARRIS AUTH OR OF "THE A B C OF WIRELE SS " R E-C EI\·I~ G A \':I R EL l':': SS C c:' .''':CERT \\Tf1r :\ HO]\IE-l\[.-\DE C RYSTAL \;ECEI\ -EI~ LONDON THE WIRELESS PRESS, LTD. t 2 & I3, HENRIETTA STREET, w.e. 2 A HOME- MADE C R Y ST AL RECEIVER WITH ADJUSTME NTS F OR B R OADCAST 'NAVE-LE N GTHS A N D E I F F EL T OW E R TIME SI GN ALS. I N ST R UCTIONS FOR BUILDING T H I S S E T ARE G IVEN IN CHAP T E R X , CRYSTAL RECEIVERS FOR BROADCAST RECEPTION BY PERCY \Y HARIUS A UTHOR OF "THE A 13 C OF W I R ELESS," ETC. LOND ON THE WIRELESS PRESS, LTD. 1 2 & 13, HENRIETTA STREET, W.c. 2 NEW YORK: ,\VIlmLESS PRESS INC., 326 BIWADWAY THE WIRELESS PRESS, LTD. FOREIGN AND CO LOAIAL AGEiVCIES: SYDNEY, N.S.vV.: 97, Clarence Street. MELBOURNE: 422 (4, Little CoUins Street. MADRID: La Prensa Radiotelegrafica, 43, Calle de Alcala. GENOA: Agenzia Radiotelegrafica Italiana, Via Varese 3. AMSTERDAM: Nederlandsch Persbureau Radio, 562, Keizersgracht. INTRODUCTION THE advent of broadcast radio-telephony has aroused con siderable interest in the simple forms of wireless receiver, with the result that the crystal detector, \vhich was fast being ousted by the thermionic valve, has once again become popular. Numerous crystal receivers are now on the market, and the beginner in wireless may well feel some con fusion as to their merits. -
The Early Years of the Telephone
©2012 JSR The early years of the telephone The early years of the telephone John S. Reid Before Bell Ask who invented the telephone and most people who have an answer will reply Alexander Graham Bell, and probably clock it up as yet another invention by a Scotsman that was commercialised beyond our borders. Like many one line summaries, this is partly true but it credits to one person much more than he really deserves. Bell didn’t invent the word, he didn’t invent the concept, what ever the patent courts decreed, and actually didn’t invent most of the technology needed to turn the telephone into a business or household reality. He did, though, submit a crucial patent at just the right time in 1876, find backers to develop his concept, promoted his invention vigorously and pursued others through the courts to establish close to a monopoly business that made him and a good many others very well off. So, what is the fuller story of the early years of the telephone? In the 1820s, Charles Wheatstone who would later make a big name for himself as an inventor of telegraphy equipment invented a device he called a ‘telephone’ for transmitting music from one room to the next. It was not electrical but relied on conducting sound through a rod. In the same decade he also invented a device he called a ‘microphone’, for listening to faint sounds, but again it was not electrical. In succeeding decades quite a number of different devices by various inventors were given the name ‘telephone’. -
Method of Accommodating for Carbon/Electret Telephone Set Variability in Automatic Speaker Verification
Europaisches Patentamt 19 European Patent Office Office europeen des brevets © Publication number: 0 654 781 A2 12 EUROPEAN PATENT APPLICATION @ Application number: 94308231.3 @ Int. CI.6: G10L 5/06 (22) Date of filing : 09.11.94 (So) Priority: 19.11.93 US 155973 @ Inventor: Sachs, Richard M. 64 Sunset Place @ Date of publication of application : Middletown, New Jersey 07748 (US) 24.05.95 Bulletin 95/21 Inventor : Schoeffler, Max S. 17 Kenwood Lane @ Designated Contracting States : Matawan, New Jersey 07747 (US) DE ES FR GB IT (74) Representative : Watts, Christopher Malcolm @ Applicant : AT & T Corp. Kelway, Dr. et al 32 Avenue of the Americas AT&T (UK) Ltd. New York, NY 10013-2412 (US) 5, Mornington Road Woodford Green Essex, IG8 0TU (GB) (S) Method of accommodating for carbon/electret telephone set variability in automatic speaker verification. In verification method of (57) a speaker system, a FIG. 6 compensating for differences in speech sam- ples obtained during registration and those obtained during verification due to the use of VERIFICATION (4-WAY) different types of microphones is provided by ,601 at least of the such that filtering one samples PROMPT the similarities of the two samples are in- creased. The filtered sample is used within the ,604 speaker verification matching process. A two- RECEIVE VERIFICATION way comparison is disclosed in which both a SPEECH SAMPLE verification speech sample and a reference sample are filtered with nonlinear microphone r609 ,606 characteristics such as carbon microphone PRODUCE CARBON characteristics. A is also VERIFICATION FILTER four-way comparison PATTERN SAMPLE disclosed in which patterns produced from un- filtered verification and reference samples and 611 from the filtered verification PRODUCE CARBON patterns produced FILTERED and reference samples are compared to identify VERIFICATION a match. -
Heterodyne Detector for Measuring the Characteristic of Elliptically Polarized Microwaves
Downloaded from orbit.dtu.dk on: Oct 02, 2021 Heterodyne detector for measuring the characteristic of elliptically polarized microwaves Leipold, Frank; Nielsen, Stefan Kragh; Michelsen, Susanne Published in: Review of Scientific Instruments Link to article, DOI: 10.1063/1.2937651 Publication date: 2008 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Leipold, F., Nielsen, S. K., & Michelsen, S. (2008). Heterodyne detector for measuring the characteristic of elliptically polarized microwaves. Review of Scientific Instruments, 79(6), 065103. https://doi.org/10.1063/1.2937651 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. REVIEW OF SCIENTIFIC INSTRUMENTS 79, 065103 ͑2008͒ Heterodyne detector for measuring the characteristic of elliptically polarized microwaves Frank Leipold, Stefan Nielsen, and Susanne Michelsen Association EURATOM, Risø National Laboratory, Technical University of Denmark, OPL-128, Frederiksborgvej 399, 4000 Roskilde, Denmark ͑Received 28 January 2008; accepted 6 May 2008; published online 4 June 2008͒ In the present paper, a device is introduced, which is capable of determining the three characteristic parameters of elliptically polarized light ͑ellipticity, angle of ellipticity, and direction of rotation͒ for microwave radiation at a frequency of 110 GHz. -
Before Valve Amplification) Page 1 of 15 Before Valve Amplification - Wireless Communication of an Early Era
(Before Valve Amplification) Page 1 of 15 Before Valve Amplification - Wireless Communication of an Early Era by Lloyd Butler VK5BR At the turn of the century there were no amplifier valves and no transistors, but radio communication across the ocean had been established. Now we look back and see how it was done and discuss the equipment used. (Orininally published in the journal "Amateur Radio", July 1986) INTRODUCTION In the complex electronics world of today, where thousands of transistors junctions are placed on a single silicon chip, we regard even electron tube amplification as being from a bygone era. We tend to associate the early development of radio around the electron tube as an amplifier, but we should not forget that the pioneers had established radio communications before that device had been discovered. This article examines some of the equipment used for radio (or should we say wireless) communications of that day. Discussion will concentrate on the equipment used and associated circuit descriptions rather than the history of its development. Anyone interested in history is referred to a thesis The Historical Development of Radio Communications by J R Cox VK6NJ published as a series in Amateur Radio, from December 1964 to June 1965. Over the years, some of the early terms used have given-way to other commonly used ones. Radio was called wireless, and still is to some extent. For example, it is still found in the name of our own representative body, the W1A. Electro Magnetic (EM) Waves were called hertzian waves or ether waves and the medium which supported them was known as the ether. -
History of Diode
HISTORY OF DIODE In electronics, a diode is a two-terminal electronic component that conducts electric current in only one direction. The term usually refers to a semiconductor diode, the most common type today, which is a crystal of semiconductor connected to two electrical terminals, a P-N junction. A vacuum tube diode, now little used, is a vacuum tube with two electrodes; a plate and a cathode. The most common function of a diode is to allow an electric current in one direction (called the diode's forward direction) while blocking current in the opposite direction (the reverse direction). Thus, the diode can be thought of as an electronic version of a check valve. This unidirectional behavior is called rectification, and is used to convert alternating current to direct current, and extract modulation from radio signals in radio receivers. However, diodes can have more complicated behavior than this simple on-off action, due to their complex non-linear electrical characteristics, which can be tailored by varying the construction of their P-N junction. These are exploited in special purpose diodes that perform many different functions. Diodes are used to regulate voltage (Zener diodes), electronically tune radio and TV receivers (varactor diodes), generate radio frequency oscillations (tunnel diodes), and produce light (light emitting diodes). Diodes were the first semiconductor electronic devices. The discovery of crystals' rectifying abilities was made by German physicist Ferdinand Braun in 1874. The first semiconductor diodes, called cat's whisker diodes were made of crystals of minerals such as galena. Today most diodes are made of silicon, but other semiconductors such as germanium are sometimes used. -
EECS 117A Demonstration 2 Microwave Measurement Instruments
University of California, Berkeley Spring 2007 EECS 117 Prof. A. Niknejad EECS 117A Demonstration 2 Microwave Measurement Instruments NAME Introduction. Please review the general sinusoidal wave concepts in Secs. 3.1–3.9 of Inan & Inan. Note carefully Section 3.3. In this demonstration you will learn how to use a “50 ohm” slotted line, crystal detector, and standing wave ratio meter to obtain the wavelength λ and voltage standing wave ratio S on a coaxial transmission line. In a later demonstration you will use these techniques to measure and control impedances and reflection coefficients on a microwave transmission system. The apparatus used is shown below. The slotted line is a (rigid) continuation of the coaxial transmission lines “a” connected at each end. It has a thin slot in its outer conductor, cut along z. A probe rides within (but not touching) the slot to sample the transmission line voltage. The probe can be moved along z, and can also be moved into and out of the slot by means of a micrometer. The probe is connected to a crystal (diode) detector that converts the time-varying microwave voltage to dc. The dc voltage is measured using the standing wave ratio (SWR) meter. MICROMETER HP 415D b SWR METER DETECTOR TUNER HP 612 A UHF SIGNAL a TERMINATION GENERATOR a GR SLOTTED LINE POINT (LOAD) Z = 0 Z Suppose a sinusoidal voltage wave j(ωt−βz) v+(t) = Re hV+ e i (1) travels from the RF generator through the slotted line and is incident on a load (resistor, capacitor etc.) at z = 0.