UNIT-3 Part A. 2. What is radio sonde? [ N/D-16]

Similar documents
Lecture 17 Microwave Tubes: Part I

RF Power Generation II

A HIGH POWER LONG PULSE HIGH EFFICIENCY MULTI BEAM KLYSTRON

DESIGN AND PERFORMANCE OF L-BAND AND S-BAND MULTI BEAM KLYSTRONS

Klystron Tubes. Two forms of such a device, also called linear beam klystron, are given in the following figure.

RF Solutions for Science.

Design, Fabrication and Testing of Gun-Collector Test Module for 6 MW Peak, 24 kw Average Power, S-Band Klystron

Detailed Design Report

INTERNATIONAL JOURNAL OF ELECTRONICS AND COMMUNICATION ENGINEERING & TECHNOLOGY (IJECET)

Development of High Power Vacuum Tubes for Accelerators and Plasma Heating

Pulsed Klystrons for Next Generation Neutron Sources Edward L. Eisen - CPI, Inc. Palo Alto, CA, USA

Development of Multiple Beam Guns for High Power RF Sources for Accelerators and Colliders

TECHNICAL SPECIFICATION Multi-beam S-band Klystron type BT267

Elements of a Television System

High-power klystrons. The benchmark in scientific research. State-of-the-art RF sources for your accelerator

This work was supported by FINEP (Research and Projects Financing) under contract

CHAPTER 4 OSCILLOSCOPES

SECTION I INTRODUCTION

14 GHz, 2.2 kw KLYSTRON GENERATOR GKP 22KP 14GHz WR62 3x400V

Available online Journal of Scientific and Engineering Research, 2018, 5(5): Research Article

18 GHz, 2.2 kw KLYSTRON GENERATOR GKP 24KP 18GHz WR62 3x400V

Presented by: Amany Mohamed Yara Naguib May Mohamed Sara Mahmoud Maha Ali. Supervised by: Dr.Mohamed Abd El Ghany

ECE 5765 Modern Communication Fall 2005, UMD Experiment 10: PRBS Messages, Eye Patterns & Noise Simulation using PRBS

DESIGN AND TECHNOLOGICAL ASPECTS OF KLYSTRON DEVELOPMENT

CATHODE-RAY OSCILLOSCOPE (CRO)

PAST EXAM PAPER & MEMO N3 ABOUT THE QUESTION PAPERS:

A tapered multi-gap multi-aperture pseudospark-sourced electron gun based X-band slow wave oscillator

CATHODE RAY OSCILLOSCOPE. Basic block diagrams Principle of operation Measurement of voltage, current and frequency

Particle-in-cell simulation study of PCE-gun for different hollow cathode aperture sizes

Tutorial: Trak design of an electron injector for a coupled-cavity linear accelerator

CHAPTER 3 OSCILLOSCOPES AND SIGNAL GENERATOR

INFN School on Electron Accelerators. RF Power Sources and Distribution

TOSHIBA Industrial Magnetron E3328

Low-Noise, High-Efficiency and High-Quality Magnetron for Microwave Oven

IOT RF Power Sources for Pulsed and CW Linacs

Pseudospark-sourced Micro-sized Electron Beams for High Frequency klystron Applications

Design and Simulation of High Power RF Modulated Triode Electron Gun. A. Poursaleh

Defense Technical Information Center Compilation Part Notice

The Cathode Ray Tube

A New 4MW LHCD System for EAST

KLYSTRON GUN ARCING AND MODULATOR PROTECTION

2 Work Package and Work Unit descriptions. 2.8 WP8: RF Systems (R. Ruber, Uppsala)

These are used for producing a narrow and sharply focus beam of electrons.

DEVELOPMENT OF X-BAND KLYSTRON TECHNOLOGY AT SLAC

LaserPXIe Series. Tunable Laser Source PRELIMINARY SPEC SHEET

M.G.M.'S COLLEGE OF ENGG. NANDED. DEPT OF ECT QUESTION BANK NO:- 1 CLASS:-BE(ECT) SUB:-DVD DATE: / /...

Klystron Lifetime Management System

Calibrate, Characterize and Emulate Systems Using RFXpress in AWG Series

DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING QUESTION BANK

Microwave Laboratory

Quartzlock Model A7-MX Close-in Phase Noise Measurement & Ultra Low Noise Allan Variance, Phase/Frequency Comparison

CHAPTER 4: HIGH ENERGY X-RAY GENERATORS: LINEAR ACCELERATORS. Jason Matney, MS, PhD

SLAC-PUB-2380 August 1979 (A)

Solid State Modulators for X-Band Accelerators

North Damping Ring RF

PHGN 480 Laser Physics Lab 4: HeNe resonator mode properties 1. Observation of higher-order modes:

Synthesized Block Up- and Downconverter Indoor / Outdoor

RF POWER GENERATION FOR FUTURE LINEAR COLLIDERS* 1. Introduction

Svetlana 3CX10,000A7/8160

NEW METHOD FOR KLYSTRON MODELING

Chapter 6: Real-Time Image Formation

CONTENTS GROUND SEGMENT FREQUENCIES MEDIUM-SIZED STATIONS LARGE STATIONS TYPES OF GROUND STATIONS

OTR-3550 FREQUENCY AGILE - F.C.C. COMPATIBLE TELEVISION PROCESSOR INSTRUCTION MANUAL

Recent ITER-Relevant Gyrotron Tests

RF plans for ESS. Morten Jensen. ESLS-RF 2013 Berlin

Chris Gilmour Studies into the Design of a Higher Efficiency Ku Band ring-loop Travelling Wave Tube SWS using the CST PIC Software.

The. Radio History. How and Why Quincy, IL Became the Digital Capitol of the World. By Tom Yingst

Swept-tuned spectrum analyzer. Gianfranco Miele, Ph.D

Techniques for Extending Real-Time Oscilloscope Bandwidth

Dark current and multipacting trajectories simulations for the RF Photo Gun at PITZ

FREQUENCY CONVERTER 1/3 RACK-MOUNTED BLOCK CONVERTER. Narda-MITEQ FEATURES OPTIONS. Unit shown with Option 17. Unit shown without Option 17

PEP-I1 RF Feedback System Simulation

Satellite Up- and Downconverter Indoor / Outdoor

Empirical Model For ESS Klystron Cathode Voltage

Final Report. U.S. Department of Energy Grant Number DE-FG02-04ER83916

TEST RESULTS OF THE 84 GHZ / 200 KW / CW GYROTRON

A SHEET-BEAM KLYSTRON PAPER DESIGN

Advanced Techniques for Spurious Measurements with R&S FSW-K50 White Paper

4.4 Injector Linear Accelerator

ADVANCED HIGH-POWER MICROWAVE VACUUM ELECTRON DEVICE DEVELOPMENT

TWO BUNCHES WITH NS-SEPARATION WITH LCLS*

Department of Electronics and Communication Engineering Shrinathji Institute of Technology & Engineering, Nathdwara (Raj.)

Critical Benefits of Cooled DFB Lasers for RF over Fiber Optics Transmission Provided by OPTICAL ZONU CORPORATION

INTEGRATED CIRCUITS DATA SHEET. TDA4510 PAL decoder. Product specification File under Integrated Circuits, IC02

FPGA IMPLEMENTATION AN ALGORITHM TO ESTIMATE THE PROXIMITY OF A MOVING TARGET

CPI Gyrotrons For Fusion EC Heating

DEVELOPMENT OF A 10 MW SHEET BEAM KLYSTRON FOR THE ILC*

decodes it along with the normal intensity signal, to determine how to modulate the three colour beams.

Limitations of a Load Pull System

Emcore SITU2831 Externally Modulated RF Amplified Fiber Optic Transmitter and SIRU3000 Fiber Optic Receiver

Application Note #63 Field Analyzers in EMC Radiated Immunity Testing

MTI-2100 FOTONIC SENSOR. High resolution, non-contact. measurement of vibration. and displacement

Experimental Results of the Coaxial Multipactor Experiment. T.P. Graves, B. LaBombard, S.J. Wukitch, I.H. Hutchinson PSFC-MIT

L-Band Block Upconverter MKT-74 Rev B JULY 2017 Page 1 of 7

Development of high power gyrotron and EC technologies for ITER

Instrumentation Grade RF & Microwave Subsystems

OSCILLOSCOPE AND DIGITAL MULTIMETER

Operating Experience and Reliability Improvements on the 5 kw CW Klystron at Jefferson Lab

45 MW, 22.8 GHz Second-Harmonic Multiplier for High-Gradient Tests*

Intelsat-29e Interference Mitigation Testing Interference Scenarios and Mitigation Techniques Enabled by the Intelsat Epic NG Class Satellites

Transcription:

UNIT-3 Part A 1. What is CFAR loss? [ N/D-16] Constant false alarm rate (CFAR) is a property of threshold or gain control devices that maintain an approximately constant rate of false target detections when the noise, and/or clutter levels, and/or ECM ( electronic counter measures) into the detector are variable. 2. What is radio sonde? [ N/D-16] A radiosonde is a battery-powered telemetry instrument package carried into the atmosphere usually by a weather balloon that measures various atmospheric parameters and transmits them by radio to a ground receiver. Modern radiosondes measure or calculate the following variables: altitude, pressure, temperature, relative humidity, wind ( both wind speed and wind direction) cosmic ray readings readings at high altitude and geographical position ( latitude/ longitude). Radiosondes measuring ozone concentration are known as ozonesondes.

Part B 1. Explain in detail about RADAR Signal Management. (16) [ N/D-16] Signal management includes everything with the waveforms and their processing that is required for radar to do its job of detecting and locating targets and determining something about the nature. Signal management starts with the design of signal waveform and its radiation in space, the collection by the receiver of echo signals reflected from targets and other objects, the use of signal processing to extract the desired signal and reject undesired echoes, the use of data processing to extract information about the detected signals, and keeping within the resources and constraints that affect signals and their management. Component parts of Radar Signal management: Signal Processing: This is the processing for the purpose of detecting desired echo signals and rejecting noise, and undesired echoes from clutter. It includes the following Matched filter To maximum the signal to noise ratio at the output of the radar receiver, and thus maximize delectability of echo signals.

Detector I Integrator The means for processing in a convenient and efficient manner the number of pulse receiver from a target so as to take full advantage of the total signal energy received from a target. Clutter reduction To eliminate or reduce unwanted clutter by one or more methods of which filtering of moving targets based on the Doppler frequency shift is the most important. CFAR: CFAR is used to maintain a constant false alarm rate at the output of the threshold detector when the radar cannot eliminate unwanted echoes. Electromagnetic compatibility The elimination of interference from other radars and other electromagnetic radiations that can enter the radar receiver is referred to as electromagnetic compatibility. Electronic counter countermeasure (ECCM) In military radar, these methods employed to reduce or eliminate the effectiveness of jamming, deception, and other hostile electronic active and passive measures whose purpose is to degrade radar performance. Threshold detection The decision as to whether the output of the radar is a desired signal. Data processing: These are the processes that take place after the detection of the desired signals for the purpose of acquiring further information about the target. Target locating: In range, angle and sometimes radial velocity. Location information is not generally thought of as either signal processing or data processing. Target trajectory: The recognition of the type of target is being viewed by the radar. It might include the recognition of aircraft from birds, one type of aircraft or ship from another, recognition of various types of weather, and information about the land and sea environment. Weapon control: In military systems, the use of the radar output for the control and guidance of weapons. Waveform design: The selection of the waveform depends on what is required of the radar for detection in noise, clutter, interference, and electronic counter counter measures as well as for the extraction of information from the radar signal. Waveform design will affect the signal and data processing.

Antenna: This is not just for radiating and collecting radar signals, but is the means by which angle information is obtained and by which the radar coverage is achieved. The antenna can act as a spatial filter that can affect the spectral properties of wideband signals. Resources of signal management: The radar engineer has available the following resources for pursuing the management of signals and extraction of information. Energy: Sufficiently large transmitted energy is important for detection of weak signals in noise at long range for obtaining accurate radar measurements. Bandwidth: This is the classical measure of information and is especially important for accurate range measurement and the temporal resolution of targets. Time: Time is necessary for accurate measurement of the Doppler frequency. Space: This applies to the physical aperture area required for an antenna. The lager the antenna aperture, the greater the echo energy at the receiver.

2. Discuss in detail about Linear Beam Power Tubes. (16) [ N/D-16] In the linear beam tubes, the electrons emitted from the cathode are formed into a long cylindrical beam that receives the full potential energy of the electric field before the beam enters the RF interaction region. Example of Linear wave tube: The klystron, traveling wave tube, klystron and extended interaction amplifier are the examples of linear beam tubes. The last two are basically hybrid devices that combine the technology of the klystron with the RF structure of the TWT. An axial magnetic field is used in the linear- beam tubes to confine the electron beam and keep electrons from hitting the RF structure. Linear beam tubes can produce much higher power than other power sources. Klystrons are capable of more than a megawatt of average power. High power is result in part, of their larger size and high voltages. A sketch of the principal parts of klystron is shown below. At the left is the cathode which emits a stream of electrons that is formed into a narrow cylindrical beam by the electron gun. The electron gun consists of other beam control electrode to provide a means for turing the beam on and off to generate pulses, and the anode. The multiple RF cavities, which corresponds to the LC resonant circuits of conventional lower frequency amplifiers, are at a note potential electrons are

not intentionally collected by the anode, as in some other tubes: instead they are removed by the collector electrode after the beam has given up its RF energy to the output RF cavity. Operation: The RF input signal is applied across the interaction gap of the first cavity. Those electrons arrive at the gap when the input signal voltage is maximum experience a voltage greater than those electrons which arrive at the gap when the input is minimum Thus the electrons that see the peak of the sine wave are speeded up and those that trough are slowed down. The process whereby some electrons are speeded up and others slowed down is called velocity modulation of the electron beam. In the drift space, electrons that are speeded up during the peak of one cycle catch up with those slowed down during the previous cycle. The result is that the electrons of the velocity- modulated beam become bunched or density modulated, after travelling through the drift space. A klystron usually has one or more appropriately placed intermediate cavities to enhance the bunching of the electron beam, which increases the gain. If the interaction gap of the output cavity is placed at the point of maximum bunching, power can be extracted from the density-modulated beam. The gain of the klystron might be 15 to 20 db per stage when synchronously tuned, so that a fourcavity klystron might provide over 50 db gain. After the bunched electron beam delivers its RF power to the output cavity, the energy of the electron beam that remains is dissipated when the spent electrons are removed by the collector. The energy dissipated by the collector is the energy lost and reduces the efficient of the tube. If the collector is insulated from the body of the tube and a negative voltage is applied to the collector, the electrons in the spent beam will have lower kinetic energy so that less heat is produced when they impact upon the collector. This results in an increase in the efficiency of the tube. Figure shows a single stage collector, but both the klystron and TWT usually employ multiplestage depressed collectors for greater efficiency. The multiple stages are intermediate voltages, which allow catching the spent electrons at a voltage near optimum. Bandwidth of a klystron: The frequency of a klystron is determined by its resonant cavities. When all are turned to the same frequency, the gain the tube is high, but the bandwidth is narrow, usually a fraction of one percent for a tube of modest power output. This is synchronous tuning. To maximize the klystron s efficiency the next to last cavity is tuned upward in frequency and is outside the pass band. Although the gain is reduced by about 10 db, the improved electron bunching results in greater efficiency and is 15 to 25 percent more output power. Broad banding of a multi cavity klystron may be accomplished by stagger tuning cavities, similar to the method for broad banding a conventional multistage IF amplifier. When stagger tuned it has a 77 MHZ bandwidth and a gain of 44 db.

Theory shows that bandwidth of klystron can be significantly increased by increasing its power and its beam preveance. Frequency changing to tuning: Conventional narrow band klystron may have their frequency changed mechanically over a relatively wide frequency range. The individual cavities of a klystron be changed in frequency by having a flexible wall in the resonant cavity, by a movable cavity element in the cavity or by a sliding contact movable cavity wall. Channel tuner mechanism: It avoids the problem of frequency tracking of the resonant cavities by pre tuning the cavities, generally at the factory. The tuning information is stored mechanically within the tuner mechanism. When a particular frequency is selected, the tuner mechanism provides the correct tuner position for each cavity to furnish the desired klystron frequency response. The tuning plungers can be actuated manually or remotely by push buttons and a servomotor. The frequency can be changed in seconds. Power: Some of the highest power radar, transmitters have used klystrons. The ability of a klystron to produce higher power than other microwave power sources is, in part, due to its geometry. The region of beam formation, RF interaction, and beam collection are separate. Efficiency: RF efficiency ( percent) = 90 20 * micro preveance. Reliability and life: High power transmitters employing power vacuum tubes have sometimes had the unwarranted reputation for poor reliability and short life. An S- Band klystron: It was a six-cavity tube tunable from 2.7 to 2.9 GHz, the frequency band reserved for air- traffic control radar. It had a peak power of from 0.5 to 2 MW, average power of from 0.5 to 3.5 KW, 50 db gain, 45% efficiency, and one db bandwidth of 39 MHz. Travelling Wave Tubes: Like the klystron, the travelling wave tube is also a linear beam tube with the cathode, RF circuit, and collector separated from one of another. The klystron and TWT were invented at different times in different parts of the world, but they are similar to one another. there is continuous interaction of the electron beam and the RF field over the entire length of the propagating strut are of the traveling wave tube. In the klystron, on the other hand the interaction occurs only at the gaps of a relatively few resonant cavities. The chief characteristic of a TWT is that, it has wide bandwidth. The major parts of a TWT are indicated below. Both the TWT and the klystron employ the principle of velocity modulation to cause the electron beam current to be periodically bunched.

The electron beam passes through the RF interaction circuit known as the slow wave structure or periodic delay line. Rabit-ear Oscillation: In some travelling wave tubes with coupled cavity circuits, oscillations appear for an instant during the turn on and turn-off portions of the pulse. These are called rabit-ear oscillation because of their characteristic appearance when the RF envelope of the pulse waveform is displayed visually on a CRT. Hybrid variants of the klystron: By combining the various features of the klystron and the traveling wave tube, an RF power source can be obtained which has bandwidth, efficiency, and gain flatness better than either the conventional klystron or TWT. This is achieved by replacing one or more of the klystron cavity circuits used in traveling wave tubes. There have been three variants of the klystron in which this is done; the Twystron, the extended interaction klystron, and clustered cavity klystron.