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Army Radio Communication in the Great War Keith R Thrower, OBE
Army radio communication in the Great War Keith R Thrower, OBE Introduction Prior to the outbreak of WW1 in August 1914 many of the techniques to be used in later years for radio communications had already been invented, although most were still at an early stage of practical application. Radio transmitters at that time were predominantly using spark discharge from a high voltage induction coil, which created a series of damped oscillations in an associated tuned circuit at the rate of the spark discharge. The transmitted signal was noisy and rich in harmonics and spread widely over the radio spectrum. The ideal transmission was a continuous wave (CW) and there were three methods for producing this: 1. From an HF alternator, the practical design of which was made by the US General Electric engineer Ernst Alexanderson, initially based on a specification by Reginald Fessenden. These alternators were primarily intended for high-power, long-wave transmission and not suitable for use on the battlefield. 2. Arc generator, the practical form of which was invented by Valdemar Poulsen in 1902. Again the transmitters were high power and not suitable for battlefield use. 3. Valve oscillator, which was invented by the German engineer, Alexander Meissner, and patented in April 1913. Several important circuits using valves had been produced by 1914. These include: (a) the heterodyne, an oscillator circuit used to mix with an incoming continuous wave signal and beat it down to an audible note; (b) the detector, to extract the audio signal from the high frequency carrier; (c) the amplifier, both for the incoming high frequency signal and the detected audio or the beat signal from the heterodyne receiver; (d) regenerative feedback from the output of the detector or RF amplifier to its input, which had the effect of sharpening the tuning and increasing the amplification. -
The Stage Is Set
The Stage Is Set: Developments before 1900 Leading to Practical Wireless Communication Darrel T. Emerson National Radio Astronomy Observatory1, 949 N. Cherry Avenue, Tucson, AZ 85721 In 1909, Guglielmo Marconi and Carl Ferdinand Braun were awarded the Nobel Prize in Physics "in recognition of their contributions to the development of wireless telegraphy." In the Nobel Prize Presentation Speech by the President of the Royal Swedish Academy of Sciences [1], tribute was first paid to the earlier theorists and experimentalists. “It was Faraday with his unique penetrating power of mind, who first suspected a close connection between the phenomena of light and electricity, and it was Maxwell who transformed his bold concepts and thoughts into mathematical language, and finally, it was Hertz who through his classical experiments showed that the new ideas as to the nature of electricity and light had a real basis in fact.” These and many other scientists set the stage for the rapid development of wireless communication starting in the last decade of the 19th century. I. INTRODUCTION A key factor in the development of wireless communication, as opposed to pure research into the science of electromagnetic waves and phenomena, was simply the motivation to make it work. More than anyone else, Marconi was to provide that. However, for the possibility of wireless communication to be treated as a serious possibility in the first place and for it to be able to develop, there had to be an adequate theoretical and technological background. Electromagnetic theory, itself based on earlier experiment and theory, had to be sufficiently developed that 1. -
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. -
Crystal Radio Set Systems: Design, Measurement, and Improvement Volume II a Web Book by Ben Tongue
Crystal Radio Set Systems: Design, Measurement, and Improvement Volume II A web book by Ben Tongue First published: 10 Jul 1999; Revised: 01/06/10 i NOTES: ii 185 PREFACE Note: An easy way to use a DVM ohmmeter to check if a ferrite is made of MnZn of NiZn material is to place the leads of the ohmmeter on a bare part of the test ferrite and read the The main purpose of these Articles is to show how resistance. The resistance of NiZn will be so high that the Engineering Principles may be applied to the design of crystal ohmmeter will show an open circuit. If the ferrite is of the radios. Measurement techniques and actual measurements are MnZn type, the ohmmeter will show a reading. The reading described. They relate to selectivity, sensitivity, inductor (coil) was about 100k ohms on the ferrite rods used here. and capacitor Q (quality factor), impedance matching, the diode SPICE parameters saturation current and ideality factor, #29 Published: 10/07/2006; Revised: 01/07/08 audio transformer characteristics, earphone and antenna to ground system parameters. The design of some crystal radios that embody these principles are shown, along with performance measurements. Some original technical concepts such as the linear-to-square-law crossover point of a diode detector, contra-wound inductors and the 'benny' are presented. Please note: If any terms or concepts used here are unclear or obscure, please check out Article # 00 for possible explanations. If there still is a problem, e-mail me and I'll try to assist (Use the link below to the Front Page for my Email address). -
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 Development of the Coherer * and Some Theories of Coherer Action
268 SCIENTIFIC AMERICAN SUPPLEMENT No. 2 182 October 27, 1917 The Development of the Coherer * And Some Theories of Coherer Action By E. C. Green THE electric wave detecting device, first known as a Branly observed that the same effect occurred in the were exhibited. Lodge was the first to give the name Branly tube and later as a coherer, has been the subject case of two slightly oxidized steel or copper wires crossed Coherer to the Branly tube, a follows: "A coherer is of much research. Many experimentalists in past years in light contact, and further observed that this contact a device in which a loose or imperfect conducting contact noticed that a number of metals, when powdered, were resistance dropped from several thousand ohms to a few between pieces of metal is improved in conductivity by the practically non-conductors when a small electromotive ohms when an electric spark was produced many yards impact on it of electric radiation." Lodge's lecture force was impressed on the loosely compressed particles, away. caused widespread interest in Branly's discove"'ies and while they became good conductors when a high electro Branly's work did not secure the notice it deserved pointed out more forcibly that a new and highly sensitive motive force was applied. until 1892 when Dr. Dawson Turner described Branly's means of detecting electric radiation had been evolved. This knowledge can be traced as far back as 1835 to experiments and his own additions to them, at a meeting The coherer used by Lodg consisted of a glass tube Monk of Rosenschceld' who described the permanent of the British Association in Edinburgh." 1 cm. -
Optimization of Low Frequency Litz-Wire RF Coils
Optimization of Low Frequency Litz-wire RF Coils J.A. Croon, II. M. fkJrSbooll1, A. F. Mehlkopf Fi7culty of Applied Physics, DeFt IJniversity of Technology, P.O. Box 5046, 2600 GA Delft, 77zeNetherlands INTRODUCTION Equations ]4] and [5] show that the skin losses are proportional to the In MRI the patient or sample losses increase with the square of the resistivity while the proximity losses are proportional to the conductiv- resonance frequency. This makes coil losses significant at low field ity. The rota1 losses are minimized if the derivative of P,,,, to p is zero. strengths. dP,oss %kin Rprox_ It is well known (1) that for frequencies of several hundreds of l&z - =--- - 0 or Rski,, = R WI stranded or litz wires can have lower losses than conventional wires, do P P PYqX Here we will investigate and present the optimization of copper solenoid coils for room temperature and for liquid nitrogen temperature. Thus the maximum coil quality is achieved if the skin losses equal the For litz wire coils we distinguish three types of losses: proximity losses. 1. losses within each considered strand, 2. proximity losses in the surrounding strands and RESULTS 3. eddy losses the environment of the coil (mainly determined by the The results of table 1 concern solenoids with a single litz wire and with sample losses). The losses within the considered strands are called skin six parallel litz wires. The six parallel wires are placed above each losses. We will show that the maximum coil quality is achieved if the other and twisted such that the losses in each parallel wire are the skin losses are equal to the proximity losses. -
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. -
Figure 1 Old Huge Magnetic Receiving Loop Antennas
ANTENTOP- 02- 2004, # 006 Old Receiving Magnetic Loop Antennas Igor Grigorov, RK3ZK [email protected] Receiving magnetic loop antennas were widely used in the professional radio communication from the beginning of the 20 Century. Since 1906 magnetic loop antennas were used for direction finding purposes needed for navigation of ships and planes. Later, from 20s, magnetic loop antennas were used for broadcasting reception. In the USSR in 20- 40 years of the 20 Century when broadcasting was gone on LW and MW, huge loop antennas were used on Reception Broadcasting Centers (see pages 93- 94 about USSRs RBC). Magnetic loop antennas worldwide were used for reception service radio stations working in VLW, LW and MW. The article writes up several designs of such old receiving loop antennas. LW- MW Huge Receiving Loop Fig. 2 shows a typical connection of the above mention Antennas for Broadcasting and huge magnetic receiving loop antennas designed for Direction Finding working on one fixing frequency to the receiver. To a resonance the loop A1 is tuned by lengthening coil L1 In old radio textbooks you can find description of old (sometimes two lengthening coils switched symmetrically magnetic receiving loop antennas. As a rule, old to both side of the loop were used) and variable air- magnetic receiving loop antennas had a triangle or dielectric capacitor C1. T1 did connection with antenna square shape, a side of the triangle or square had feedline. L1, C1 and T1, as a rule, are placed directly length in 10-20 meters. The huge square was put near the antenna keeping minimum length for wires from on to a corner. -
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. -
Making Radio Waves Telegraph
Making Radio Waves Telegraph Background Information What better way to demonstrate the detection of electromagnetic waves then to produce the electromagnetic waves (Radio waves) that are detected. Radio waves can be made by making a telegraph and a cohere detector can receive those radio waves. This early style telegraph generates a radio wave signal by producing a spark when the circuit is completed. Radio waves are produced by the spark. When there is a spark, electrons are transferred from one electrode to another as the electrons move, energy is transferred into heat, light, and a standing wave at the frequency of a radio wave. This allows the operator to generate radio waves by connecting and disconnecting the circuit respectively. In this design the switch is a piece of metal that is depressed to make contact, and released to open the circuit breaking the connection. (See photograph below) This circuit can be opened and closed easily in a pattern known as Morse code to send information wirelessly. A coherer detector is a historic radio wave detector made of common everyday materials. It consists of a tube containing some metal filings and two electrodes within millimeters of each other. Each electrode is connected to an observable resistor like a light bulb, speakers, or headphones. In the presence of a radio wave the metal filings form a bridge that completes a circuit. When the circuit is closed the radio wave becomes observable, success! The tube needs to be taped so that the metal filings will decoher and the detector is primed to detect another transmission. -
DESIGNING a DX CRYSTAL SET Equipment
DESIGNING A DX CRYSTAL SET by Mike Tuggle 46-469 Kuneki St. Kaneohe, HI 96744-3536 E-Mail: [email protected] Long distance reception with crystal radios is once again becoming a serious pursuit among hams and other radio hobbyists. They are discovering that the DX capabilities of these receivers have been greatly underrated. I've been particularly interested in crystal sets since 1959, when I first discovered you could actually DX with them. The Internet has aided crystal set DX activity by making exchange of ideas between like- minded enthusiasts much, much easier. This article only touches the surface from a personal perspective. The reader is encouraged to pursue the online resources, described below, covering all aspects and providing further examples of this fascinating hobby. In this article I'll cover general design considerations for building DX crystal sets, but will leave the actual construction specifications up to you. Equipment Figures 1 and 2 show an example of a DX crystal set. I call it the "Lyonodyne-17." The design evolved from an earlier version described in the November, 1978 OTB. As you can see, this is not your grandfather's crystal set. Antenna (right) and detector (left) tuners are mounted on the middle board. Wave traps are located fore and aft on separate boards, making it possible to adjust the coupling by moving the boards. The antenna coil (L1) is wound on a short ferrite rod. The matching transformer unit for my RCA "Big Cans" sound powered phones is at front, left. So, what makes a crystal radio a "DX" set? Well, this one is double-tuned (L1-C1 and L2-C2) for selectivity to tune weak DX stations in the RF jungle we now live in.