Status of the BRAMS network and recent progress

Slides:



Advertisements
Similar presentations
Stratagem EH4 Field Evaluation of Data Quality.
Advertisements

Inside the K3 High Performance Rig Design Dynamic Range is your friend! Dynamic Range is your friend! Hands on Ham Radio. © 2009 Elecraft, Inc.
Fundamentals of Data & Signals (Part II) School of Business Eastern Illinois University © Abdou Illia, Spring 2015 (February18, 2015)
Lorentz force detuning measurements on the CEA cavity
Implement a 2x2 MIMO OFDM-based channel measurement system (no data yet) at 2.4 GHz Perform baseband processing and digital up and down conversion on Nallatech.
Chapter 6 Antennas Antenna Basics
Design Review: November 17,2011 Team Members: Allan Davis Carlos Gonzalez Cooper McBride.
Noise near peak field is increased Peak width narrow Peak is symmetric Purpose: Resonate nuclei to prevent polarization. Matching the resonant frequencies.
General Licensing Class Your HF Transmitter Your organization and dates here.
Ninth Synthesis Imaging Summer School Socorro, June 15-22, 2004 Cross Correlators Walter Brisken.
Radar: Acronym for Radio Detection and Ranging
General Licensing Class G5A – G5C Electrical Principles Your organization and dates here.
Checking Antenna Systems
Solar dynamic spectra C. Vocks and G. Mann 1. Spectrum of the quiet Sun: First results 2. How to obtain spectra: Beamformed data 3. Single station spectra.
HIAPER Cloud Radar Transceiver Exciter Receiver Oscillators High-Powered Amplifier Calibration Exciter Receiver Oscillators High-Powered Amplifier Calibration.
Electromagnetic Compatibility of a DC Power Distribution System for the ATLAS Liquid Argon Calorimeter G. BLANCHOT CERN, CH-1211 Geneva 23, Switzerland.
Antenna Design Tools VE3KL
Bi-Directional RF Data Communication A Robot Control Device Team BDRFC.
1 CISCO NETWORKING ACADEMY PROGRAM (CNAP) SEMESTER 1/ MODULE 4 Cable Testing.
Technician License Course Chapter 5 Operating Station Equipment Lesson Plan Module 11: Transmitters, Receivers and Transceivers.
Basic (VHF) Radio Communications
Namaste Project 3.4 GHz Interference Study Preliminary document - Work in Progress updated The intent of this study is to collect data which may.
Distributed Adaptive Control and Metrology for Large Radar Apertures Principal Investigator: James Lux, P.E. (337) Dr. Elaine Chapin (334), Samuel Li (337),
1 of 22 Glaciers and Ice Sheets Interferometric Radar (GISIR) Center for Remote Sensing of Ice Sheets, University of Kansas, Lawrence, KS
IMC 2012 – La Palma – 21/09/2012 BRAMS, the Belgian Radio Meteor Stations : latest developments Hervé Lamy.
Andreas Horneffer for the LOPES Collaboration Detecting Radio Pulses from Air Showers with LOPES.
Amplitude Modulation 2.2 AM RECEIVERS
CHAPTER 2 Amplitude Modulation 2-3 AM RECEIVERS. Introduction AM demodulation – reverse process of AM modulation. Demodulator: converts a received modulated-
AST 443: Submm & Radio Astronomy November 18, 2003.
FIFO 64KX9 FIFO 64KX9 CLOCK D/A Converter 10 bit D/A Converter 10 bit Up-Converter LO Down ConverterIntegrator To DAQ Card 9 Bit Basic Schematic of.
Technician License Course Chapter 4 Lesson Plan Module 9 – Antenna Fundamentals, Feed Lines & SWR.
TUTORIAL BRAMS ZOO. What is a meteoroid? A meteoroid is a solid object moving in interplanetary space, of a size considerably smaller than an asteroid.
University of Kansas 2004 ITTC Summer Lecture Series Network Analyzer Operation John Paden.
CHAPTER 2 Amplitude Modulation 2-3 AM RECEIVERS. Introduction AM demodulation – reverse process of AM modulation. Demodulator: converts a received modulated-
Radio polarisation measurement of meteor trail echoes during the Perseids 2012 S. Ranvier (1), M. Anciaux (1), H. Lamy (1), J. De Keyser (1) ‏, S. Calders.
AM RECEPTION Introduction
Attenuation measurement with all 4 frozen-in SPATS strings Justin Vandenbroucke Freija Descamps IceCube Collaboration Meeting, Utrecht, Netherlands September.
CODALEMA A Cosmic Ray Radio Detection Array ICRC 2007, 3-11 July Merida, Mexico CODALEMA A Cosmic Ray Radio Detection Array Didier Lebrun, LPSC Grenoble.
BASIC INSTRUMENTS - oscilloscopes
HDTV Test Process Improvement (TOSHIBA RF) Sponsor: Aaron Foster TOSHIBA America Consumer Products, Inc. Manufacturing Division Project Team: Josue Caballero,
Duplexer Repurposing Duplexer retired from Ely PD Originally tuned to TX RX MHz Frequency separation of 3.52 MHz Retune to Gilbert TX
Antenna Basics.
FUNCTION GENERATOR.
Amplitude Modulation Part 2 - AM RECEPTION.  To define AM demodulation  To define and describe the receiver parameters  To describe the operation of.
Ch7 Operational Amplifiers and Op Amp Circuits
RFI Protection Activities in IAA RAS
Smart Attendance System
Status of the BRAMS project & plans for the future
RFI Protection Activities in IAA RAS
A Closer Look at CODAR HF Radar Spectra
Antennas 10/18/2017.
Amplitude Modulation 2-3 AM RECEIVERS
Vertical Antenna Myths
Amateur Extra Q & A Study Pool
Technician Licensing Class
Technician Licensing Class
A Portion of the SCP RF Control System LCLS Related
Technician Licensing Class
Antenna Design Tools VE3KL
Overview of major shower observations by the BRAMS network
Fundamentals of Data & Signals (Part II)
UWB Receiver Algorithm
Status of the BRAMS activities
What is the primary purpose of a dummy load?
What is a beam antenna? A. An antenna built from aluminum I-beams
FCARC Jan 11,2016.
Study of joint CAMS/BRAMS observations & comparison with simulations
Study of joint CAMS/BRAMS observations & comparison with simulations
ENEE222 Elements of Discrete Signal Analysis Lab 9 1.
Near Field Probe Configuration
Presentation transcript:

Status of the BRAMS network and recent progress H. Lamy & BRAMS team

BRAMS network : full inspection during summer / fall 2018 26 active Rx 1 Tx We solved many small (and not so small) problems

Some problems encountered Receiving stations Some problems encountered Calibrator unplugged Meinberg not using GPS NMEA to synchronize the PC Clock ICOM-R75 not using PRE-AMP2, AGC OFF or using additional functions ….

Receiving stations : vertical orientation BELEUZ Radiation pattern much more closer to theoretical one BEOVER

Receiving stations : change of azimut orientation Goal : trying to minimize local interference BEREDU

Receiving stations : impedance matching Mounting specifications of the antenna manual provided at best a return loss S11  -15 dB at f = 49.97 MHz (for most antennas it was lower) and a dip for S11 which was never at  50 MHz but more at f  50.6 – 50.7 MHz Tests in June with an antenna in Uccle to increase the length of elements by a few cm to decrease the resonance frequency of the antenna. Increase by  3 cm on each side of the 3 elements provides the best results Length of the matching element chosen to maximize the dip.  

ICOM-R75 receivers 18of them had problems with a progressive loss of sensitivity. The origin of the problem was identified by M. Anciaux who was able to repair 13 of them ICOM-R75 are not commercially produced anymore  search for new solutions using SDR receivers (see next talk)

Transmitter in Dourbes P  150 W Circular polarisation f = 49.97 MHZ Is this correct?  full characterization on 21 September

Transmitter in Dourbes Picotest G5100A Waveform generator Tomco BT00400-AlphaSA-CW Ecoflex 15 RF cable

Transmitter in Dourbes Full characterization of the Tx on 21/09/2018 using dummy load, wattmeter, oscilloscope and antenna analyzer Power amplifier characterization : using the Wattmeter in between the amplifier and the antenna, we found P_forward  110 W and P_reflected  15 W, providing a SWR  2.2. Total power at the antenna should then be of the order of 95 W. More accurate measurements using the dummy load and the oscilloscope give P_forward = 104.7 W incident on the antenna cable. Antenna characterization : Two 50 cables in parallel linked by a T  equivalent resistance (resistive part) measured at the extremity of the RF cable is  25.6  as expected. Taking into account the losses in the cable, we expect an incident power of 95.5 W at the entrance of the T Independent measurements of the adaptation of the two individual antennas: SWR=1.68 and 1.16 Ant 1 : P=44.3 W – Ant 2 : P=40.6 W,  = -96°

Transmitter in Dourbes Conclusions : We emit far less than 150 Watts ( 90 Watts) The emitted wave is not perfectly circularly polarized but not too far (96° instead of 90°) Still to do : Measurements of the radiation pattern in-situ using our drone (March?) Replacement of the current system with an improved design to guarantee 150 W emission and perfectly circularly polarized wave

BRAMS availability tool Data transfer Data from all 26 stations are now transferred via FTP 23 stations are automatically transferring the data daily using the BRAMS-FTP facility 3 stations are sending their data weekly using FileZilla 20 stations can be accessed remotely via Team Viewer or Remote Desktop. BRAMS availability tool

Quality check of the data Matlab and/or Python tools have been developed to Check for saturation Derive the amplitude and exact frequency of the calibrator Amplitude provides an estimate of the response of the front-end of the receiving station (ICOM R-75 + sound-card) Frequency provides an estimate of the frequency offset due to the poor stability of the LO of the ICOM-R75 These tools are currently being implemented to the archiving system in order to quickly identify potential problems (mostly with the receiver but also calibrator off, etc …)

Saturation of the data 01H30 07H10 Total nb of samples in a WAV file  5512 * 300  1 653 600

Saturation of the data 07H10 01H30

Saturation of the data

Saturation of the data

Amplitude and frequency of the calibrator signal First we take the FFT of the whole 5 minutes long WAV file (f fs/nfft = 1/300 Hz) We then accurately determine the frequency and amplitude of the calibrator signal. Two different techniques have been used Fit a sinc function to the FFT spectrum in the region of the calibrator frequency « Integrate » the contributions of the various FFT frequencies in a limited range of frequencies and subtract an estimate of the local noise

Method 1 : sinc fit of the FFT spectrum Works well in Humain FFT values FFT Frequency Red discrete crosses = FFT values Blue continuous curve = sinc fit

Method 1 : sinc fit of the FFT spectrum

Method 2 : « integration » of the FFT spectrum contributions The LO of the ICOM-R75 is not stabilized. Instead we locate the max of the FFT spectrum and sum the values of the FFT spectrum in a small frequency range centered on it Then we estimate the contribution of the noise in a frequency range nearby and subtract it   Based on Parseval’s theorem :

Utility of the amplitude of the calibrator signal To detect a potential problem with the ICOM-R75 (progressive decrease of amplitude over a period of time) To calibrate power measurements of meteor echoes in Watts (see talk about CAMS/BRAMS comparisons)

The meteor radar in Dourbes

The meteor radar in Dourbes

The meteor radar in Dourbes