Speed and Yaw Rate Estimation in Autonomous Vehicles Using Doppler Radar Measurements
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Chapter-5 Doppler Effect
Chapter-5 Doppler Effect Stationary source Stationary observer Moving source Stationary observer Stationary source Moving observer Moving source Moving observer http://www.astro.ubc.ca/~scharein/a311/Sim/doppler/Doppler.html Doppler Effect The Doppler effect is the apparent change in the frequency of a wave motion when there is relative motion between the source of the waves and the observer. The apparent change in frequency f experienced as a result of the Doppler effect is known as the Doppler shift. The value of the Doppler shift increases as the relative velocity v between the source and the observer increases. The Doppler effect applies to all forms of waves. Doppler Effect (Moving Source) http://www.absorblearning.com/advancedphysics/demo/units/040103.html Suppose the source moves at a steady velocity vs towards a stationary observer. The source emits sound wave with frequency f. From the diagram, we can see that the distance between crests is shortened such that ' vs Since = c/f and = 1/f, We get c c v s f ' f f c vs f ' ( ) f c vs Doppler Effect (Moving Observer) Consider an observer moving with velocity vo toward a stationary source S. The source emits a sound wave with frequency f and wavelength = c/f. The velocity of the sound wave relative to the observer is c + vo. c Doppler Shift Consider a source moving towards an observer, the Doppler shift f is c f f ' f ( ) f f c vs f v s f c v s f v If v <<c, then we get s s f c The above equation also applies to a receding source, with vs taking as negative. -
The Montague Doppler Radar, an Overview June 2018
ISSUE PAPER SERIES The Montague Doppler Radar, An Overview June 2018 NEW YORK STATE TUG HILL COMMISSION DULLES STATE OFFICE BUILDING · 317 WASHINGTON STREET · WATERTOWN, NY 13601 · (315) 785-2380 · WWW.TUGHILL.ORG The Tug Hill Commission Technical and Issue Paper Series are designed to help local officials and citizens in the Tug Hill region and other rural parts of New York State. The Tech- nical Paper Series provides guidance on procedures based on questions frequently received by the Commis- sion. The Issue Paper Series pro- vides background on key issues facing the region without taking advocacy positions. Other papers in each se- ries are available from the Tug Hill Commission. Please call us or vis- it our website for more information. The Montague Doppler Weather Radar, An Overview Table of Contents Introduction .................................................................................................................................................. 1 Who owns the Montague radar? ................................................................................................................. 1 Who uses the Montague radar? .................................................................................................................. 1 How does the radar system work? .............................................................................................................. 2 How does the radar predict lake-effect snowstorms? ................................................................................ 2 How does the -
Chapter 30: Quantum Physics ( ) ( )( ( )( ) ( )( ( )( )
Chapter 30: Quantum Physics 9. The tungsten filament in a standard light bulb can be considered a blackbody radiator. Use Wien’s Displacement Law (equation 30-1) to find the peak frequency of the radiation from the tungsten filament. −− 10 1 1 1. (a) Solve Eq. 30-1 fTpeak =×⋅(5.88 10 s K ) for the peak frequency: =×⋅(5.88 1010 s−− 1 K 1 )( 2850 K) =× 1.68 1014 Hz 2. (b) Because the peak frequency is that of infrared electromagnetic radiation, the light bulb radiates more energy in the infrared than the visible part of the spectrum. 10. The image shows two oxygen atoms oscillating back and forth, similar to a mass on a spring. The image also shows the evenly spaced energy levels of the oscillation. Use equation 13-11 to calculate the period of oscillation for the two atoms. Calculate the frequency, using equation 13-1, from the inverse of the period. Multiply the period by Planck’s constant to calculate the spacing of the energy levels. m 1. (a) Set the frequency T = 2π k equal to the inverse of the period: 1 1k 1 1215 N/m f = = = =4.792 × 1013 Hz Tm22ππ1.340× 10−26 kg 2. (b) Multiply the frequency by Planck’s constant: E==×⋅ hf (6.63 10−−34 J s)(4.792 × 1013 Hz) =× 3.18 1020 J 19. The light from a flashlight can be considered as the emission of many photons of the same frequency. The power output is equal to the number of photons emitted per second multiplied by the energy of each photon. -
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2 February 15, 2006 . DRAFT Cambridge-MIT Institute Multidisciplinary Design Project This Dictionary/Glossary of Engineering terms has been compiled to compliment the work developed as part of the Multi-disciplinary Design Project (MDP), which is a programme to develop teaching material and kits to aid the running of mechtronics projects in Universities and Schools. The project is being carried out with support from the Cambridge-MIT Institute undergraduate teaching programe. For more information about the project please visit the MDP website at http://www-mdp.eng.cam.ac.uk or contact Dr. Peter Long Prof. Alex Slocum Cambridge University Engineering Department Massachusetts Institute of Technology Trumpington Street, 77 Massachusetts Ave. Cambridge. Cambridge MA 02139-4307 CB2 1PZ. USA e-mail: [email protected] e-mail: [email protected] tel: +44 (0) 1223 332779 tel: +1 617 253 0012 For information about the CMI initiative please see Cambridge-MIT Institute website :- http://www.cambridge-mit.org CMI CMI, University of Cambridge Massachusetts Institute of Technology 10 Miller’s Yard, 77 Massachusetts Ave. Mill Lane, Cambridge MA 02139-4307 Cambridge. CB2 1RQ. USA tel: +44 (0) 1223 327207 tel. +1 617 253 7732 fax: +44 (0) 1223 765891 fax. +1 617 258 8539 . DRAFT 2 CMI-MDP Programme 1 Introduction This dictionary/glossary has not been developed as a definative work but as a useful reference book for engi- neering students to search when looking for the meaning of a word/phrase. It has been compiled from a number of existing glossaries together with a number of local additions. -
Calculus Terminology
AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential -
An Implementation of Real-Time Phased Array Radar Fundamental Functions on a DSP-Focused, High-Performance, Embedded Computing Platform
aerospace Article An Implementation of Real-Time Phased Array Radar Fundamental Functions on a DSP-Focused, High-Performance, Embedded Computing Platform Xining Yu 1,*, Yan Zhang 1, Ankit Patel 1, Allen Zahrai 2 and Mark Weber 2 1 School of Electrical and Computer Engineering, University of Oklahoma, 3190 Monitor Avenue, Norman, OK 73019, USA; [email protected] (Y.Z.); [email protected] (A.P.) 2 National Severe Storms Laboratory, National Oceanic and Atomospheric Administration, Norman, OK 73072, USA; [email protected] (A.Z.); [email protected] (M.W.) * Correspondence: [email protected]; Tel.: +1-405-325-2871 Academic Editor: Konstantinos Kontis Received: 22 July 2016; Accepted: 2 September 2016; Published: 9 September 2016 Abstract: This paper investigates the feasibility of a backend design for real-time, multiple-channel processing digital phased array system, particularly for high-performance embedded computing platforms constructed of general purpose digital signal processors. First, we obtained the lab-scale backend performance benchmark from simulating beamforming, pulse compression, and Doppler filtering based on a Micro Telecom Computing Architecture (MTCA) chassis using the Serial RapidIO protocol in backplane communication. Next, a field-scale demonstrator of a multifunctional phased array radar is emulated by using the similar configuration. Interestingly, the performance of a barebones design is compared to that of emerging tools that systematically take advantage of parallelism and multicore capabilities, including the Open Computing Language. Keywords: phased array radar; embedded computing; serial RapidIO; MPAR 1. Introduction 1.1. Real-Time, Large-Scale, Phased Array Radar Systems In [1], we had introduced the real-time phased array radar (PAR) processing based on the Micro Telecom Computing Architecture (MTCA) chassis. -
Design Trade-Offs for Airborne Phased Array Radar for Atmospheric Research
Design Trade-offs for Airborne Phased Array Radar for Atmospheric Research Jorge L. Salazar, Eric Loew, Pei-Sang Tsai, V. Chandrasekar Jothiram Vivekanandan and Wen Chau Lee Colorado State University (CSU) National Center for Atmospheric Research (NCAR) NCAR Affiliate Scientist 3450 Mitchell Lane Boulder, CO 80301, USA 1373 Fort Collins, CO 80523, U Abstract - This paper discusses the design options and trade- Besides the fact that both are single-polarized and passive offs of the key performance parameters, technology, and arrays, fast electronically scanned beams have provided the costs of dual-polarized and two-dimensional active phased scientific community with higher temporal resolution array antenna for an atmospheric airborne radar system. The measurements that improve detection and warning for severe design proposed provides high-resolution measurements of high-impact weather. Tornado false alarm rates have been the air motion and rainfall characteristics of very large storms reduced substantially and the tornado warning lead times that are difficult to observe with a ground-based radar system. extended from 14 minutes to 20 minutes [4]. Parameters such as antenna size, wavelength, beamwidth, transmit power, spatial resolution, along-track resolution, and Considering the benefit of phased array technology, polarization have been evaluated. The paper presents a academic, state, federal, and private institutions have been performance evaluation of the radar system. Preliminary working together to develop phased-array radar for results from the antenna front-end section that corresponds to atmospheric applications. Currently, the Massachusetts a Line Replacement Unit (LRU) are presented. Institute of Technology’s Lincoln Laboratory (MIT-LL) is developing a multifunction, two-dimensional (2-D), dual-pol, Index Terms – Airborne Doppler radar, ELDORA, phased flat and multifunction S-band radar system [6]. -
Calculus Formulas and Theorems
Formulas and Theorems for Reference I. Tbigonometric Formulas l. sin2d+c,cis2d:1 sec2d l*cot20:<:sc:20 +.I sin(-d) : -sitt0 t,rs(-//) = t r1sl/ : -tallH 7. sin(A* B) :sitrAcosB*silBcosA 8. : siri A cos B - siu B <:os,;l 9. cos(A+ B) - cos,4cos B - siuA siriB 10. cos(A- B) : cosA cosB + silrA sirrB 11. 2 sirrd t:osd 12. <'os20- coS2(i - siu20 : 2<'os2o - I - 1 - 2sin20 I 13. tan d : <.rft0 (:ost/ I 14. <:ol0 : sirrd tattH 1 15. (:OS I/ 1 16. cscd - ri" 6i /F tl r(. cos[I ^ -el : sitt d \l 18. -01 : COSA 215 216 Formulas and Theorems II. Differentiation Formulas !(r") - trr:"-1 Q,:I' ]tra-fg'+gf' gJ'-,f g' - * (i) ,l' ,I - (tt(.r))9'(.,') ,i;.[tyt.rt) l'' d, \ (sttt rrJ .* ('oqI' .7, tJ, \ . ./ stll lr dr. l('os J { 1a,,,t,:r) - .,' o.t "11'2 1(<,ot.r') - (,.(,2.r' Q:T rl , (sc'c:.r'J: sPl'.r tall 11 ,7, d, - (<:s<t.r,; - (ls(].]'(rot;.r fr("'),t -.'' ,1 - fr(u") o,'ltrc ,l ,, 1 ' tlll ri - (l.t' .f d,^ --: I -iAl'CSllLl'l t!.r' J1 - rz 1(Arcsi' r) : oT Il12 Formulas and Theorems 2I7 III. Integration Formulas 1. ,f "or:artC 2. [\0,-trrlrl *(' .t "r 3. [,' ,t.,: r^x| (' ,I 4. In' a,,: lL , ,' .l 111Q 5. In., a.r: .rhr.r' .r r (' ,l f 6. sirr.r d.r' - ( os.r'-t C ./ 7. /.,,.r' dr : sitr.i'| (' .t 8. tl:r:hr sec,rl+ C or ln Jccrsrl+ C ,f'r^rr f 9. -
Electrical Power and Energy
Electric Circuits Name: Electrical Power and Energy Read from Lessons 2 and 3 of the Current Electricity chapter at The Physics Classroom: http://www.physicsclassroom.com/Class/circuits/u9l2d.html http://www.physicsclassroom.com/Class/circuits/u9l3d.html MOP Connection: Electric Circuits: sublevel 3 Review: 1. The electric potential at a given location in a circuit is the amount of _____________ per ___________ at that location. The location of highest potential within a circuit is at the _______ ( +, - ) terminal of the battery. As charge moves through the external circuit from the ______ ( +, - ) to the ______ ( +, - ) terminal, the charge loses potential energy. As charge moves through the battery, it gains potential energy. The difference in electric potential between any two locations within the circuit is known as the electric potential difference; it is sometimes called the _____________________ and represented by the symbol ______. The rate at which charge moves past any point along the circuit is known as the ___________________ and is expressed with the unit ________________. The diagram at the right depicts an electric circuit in a car. The rear defroster is connected to the 12-Volt car battery. Several points are labeled along the circuit. Use this diagram for questions #2-#6. 2. Charge flowing through this circuit possesses 0 J of potential energy at point ___. 3. The overall effect of this circuit is to convert ____ energy into ____ energy. a. electrical, chemical b. chemical, mechanical c. thermal, electrical d. chemical, thermal 4. The potential energy of the charge at point A is ___ the potential energy at B. -
CMA-2012 Doppler Velocity Sensor and Navigation System
CMA-2012 Doppler Velocity Sensor and Navigation System High Accuracy Velocity Sensor Ideally Suited for Helicopter Operations The CMA-2012 Doppler Velocity Sensor and The CMA-2012’s superior accuracy and performance are Navigation System represents the culmination achieved by integrating several technologies into one compact, of CMC Electronics’ 50 years of experience in low weight unit. A frequency modulation/continuous wave (FM/CW) modulation technique, together with a four-beam Janus airborne Doppler radar and navigation systems. It configuration, is optimized for low-speed conditions. A dynamic is particularly well suited for helicopter hover and carrier breakthrough circuit lowers hover drift. Signal returns then low-speed operations, such as anti-submarine undergo digital signal processing to optimize signal acquisition warfare and SAR, and for weapons targeting during over marginal terrain, such as smooth water, sand or snow, and tactical flight manoeuvres, where the highest enhance tracking precision accuracy. Pitch, roll and yaw heading accuracy velocity sensor is required to ensure inputs further enhance the CMA-2012’s performance during mission accomplishment. dynamic helicopter movements. With the input of pitch, roll and heading information, the CMA-2012 can provide Doppler navigation system functions, compute present position and other navigation information, and output navigation data to CMC’s or other multifunction CDUs via a digital data bus. Extensive flight testing of the CMA-2012 has demonstrated its excellent performance. -
Radar Artifacts and Associated Signatures, Along with Impacts of Terrain on Data Quality
Radar Artifacts and Associated Signatures, Along with Impacts of Terrain on Data Quality 1.) Introduction: The WSR-88D (Weather Surveillance Radar designed and built in the 80s) is the most useful tool used by National Weather Service (NWS) Meteorologists to detect precipitation, calculate its motion, estimate its type (rain, snow, hail, etc) and forecast its position. Radar stands for “Radio, Detection, and Ranging”, was developed in the 1940’s and used during World War II, has gone through numerous enhancements and technological upgrades to help forecasters investigate storms with greater detail and precision. However, as our ability to detect areas of precipitation, including rotation within thunderstorms has vastly improved over the years, so has the radar’s ability to detect other significant meteorological and non meteorological artifacts. In this article we will identify these signatures, explain why and how they occur and provide examples from KTYX and KCXX of both meteorological and non meteorological data which WSR-88D detects. KTYX radar is located on the Tug Hill Plateau near Watertown, NY while, KCXX is located in Colchester, VT with both operated by the NWS in Burlington. Radar signatures to be shown include: bright banding, tornadic hook echo, low level lake boundary, hail spikes, sunset spikes, migrating birds, Route 7 traffic, wind farms, and beam blockage caused by terrain and the associated poor data sampling that occurs. 2.) How Radar Works: The WSR-88D operates by sending out directional pulses at several different elevation angles, which are microseconds long, and when the pulse intersects water droplets or other artifacts, a return signal is sent back to the radar. -
Continuous Wave Radar
Continuous Wave Radar CW radar sets transmit a high-frequency signal continuously. The echo signal is received and processed permanently. One has to resolve two problems with this principle: Figure 1: The continuous wave radar method often uses separate transmit and receive antennas. These are constructed on a double-sided printed circuit board. prevent a direct connection of the transmitted energy into the receiver (feedback connection), assign the received echoes to a time system to be able to do run time measurements. A direct connection of the transmitted energy into the receiver can be prevented by: spatial separation of the transmitting antenna and the receiving antenna, e.g. the aim is illuminated by a strong transmitter and the receiver is located in the missile flying direction towards the aim; Frequency dependent separation by the Doppler-frequency during the measurement of speeds. A run time measurement isn't necessary for speed gauges, the actual range of the delinquent car doesn't have a consequence. If you need range information, then the time measurement can be realized by a frequency modulation or phase keying of the transmitted power. A CW-radar transmitting a unmodulated power can measure the speed only by using the Doppler- effect. It cannot measure a range and it cannot differ between two or more reflecting objects. Table of content « CW-Radar » 1. Doppler Radar 2. Block diagram of CW radar Direct conversion receiver Superheterodyne 3. Applications of unmodulated continuous wave radar Speed gauges Doppler radar motion sensor Motion monitoring When an echo signal is received, then that is the proof that there is an obstacle in the propagation direction of the electromagnetic waves.