14.5mm 14.5mm

Σχετικά έγγραφα
Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee

Fundamentals of Array Antennas

General 2 2 PT -Symmetric Matrices and Jordan Blocks 1

Copyright is owned by the Author of the thesis. Permission is given for a copy to be downloaded by an individual for the purpose of research and

Homework 8 Model Solution Section

Spectrum Representation (5A) Young Won Lim 11/3/16

Development and Verification of Multi-Level Sub- Meshing Techniques of PEEC to Model High- Speed Power and Ground Plane-Pairs of PFBS

Second Order RLC Filters

Bayesian statistics. DS GA 1002 Probability and Statistics for Data Science.

ECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Decision-Making in the Dark: How Pre-Trial Errors Change the Narrative in Criminal Jury Trials

The Nottingham eprints service makes this work by researchers of the University of Nottingham available open access under the following conditions.

Πανεπιστήμιο Πειραιώς Τμήμα Πληροφορικής Πρόγραμμα Μεταπτυχιακών Σπουδών «Πληροφορική»

Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis

ExpIntegralE. Notations. Primary definition. Specific values. Traditional name. Traditional notation. Mathematica StandardForm notation

Technical Research Report, Earthquake Research Institute, the University of Tokyo, No. +-, pp. 0 +3,,**1. No ,**1

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.


encouraged to use the Version of Record that, when published, will replace this version. The most /BCJ BIOCHEMICAL JOURNAL

: Monte Carlo EM 313, Louis (1982) EM, EM Newton-Raphson, /. EM, 2 Monte Carlo EM Newton-Raphson, Monte Carlo EM, Monte Carlo EM, /. 3, Monte Carlo EM

NBER WORKING PAPER SERIES MAKING THE MOST OF CAPITAL IN THE 21ST CENTURY. Peter H. Lindert. Working Paper

CRASH COURSE IN PRECALCULUS

Section 8.3 Trigonometric Equations

Statistical Inference I Locally most powerful tests

Forced Pendulum Numerical approach

encouraged to use the Version of Record that, when published, will replace this version. The most /BCJ

Assalamu `alaikum wr. wb.

I haven t fully accepted the idea of growing older

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

Σχέση στεφανιαίας νόσου και άγχους - κατάθλιψης

Inverse trigonometric functions & General Solution of Trigonometric Equations

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

NPI Unshielded Power Inductors

6.003: Signals and Systems. Modulation

Equations. BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1. du dv. FTLI : f (B) f (A) = f dr. F dr = Green s Theorem : y da

Surface Mount Aluminum Electrolytic Capacitors

Answers - Worksheet A ALGEBRA PMT. 1 a = 7 b = 11 c = 1 3. e = 0.1 f = 0.3 g = 2 h = 10 i = 3 j = d = k = 3 1. = 1 or 0.5 l =

Sampling Basics (1B) Young Won Lim 9/21/13

ΕΙΣΑΓΩΓΗ ΣΤΗ ΣΤΑΤΙΣΤΙΚΗ ΑΝΑΛΥΣΗ

Finite Field Problems: Solutions

ΖητΗματα υποδοχης και προσληψης του Franz Kafka στην ΕλλΑδα

Εγκατάσταση λογισμικού και αναβάθμιση συσκευής Device software installation and software upgrade

Schedulability Analysis Algorithm for Timing Constraint Workflow Models

Eight Examples of Linear and Nonlinear Least Squares

ΔΥΝΑΜΙΚΗ & ΕΛΕΓΧΟΣ ΑΣΚΗΣΕΙΣ ΕΠΑΝΑΛΗΨΗΣ

ibemo Kazakhstan Republic of Kazakhstan, West Kazakhstan Oblast, Aksai, Pramzone, BKKS office complex Phone: ; Fax:

derivation of the Laplacian from rectangular to spherical coordinates

Design and Fabrication of Water Heater with Electromagnetic Induction Heating

Ελίζ Πάρσλι. For Magnolia s aunties. Για τις θείες της Μερσίνας. Hachette Book Group, 2017 / Εκδοσεισ Ψυχογιοσ, 2018

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

This is an electronic reprint of the original article. This reprint may differ from the original in pagination and typographic detail.

070-A

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

department listing department name αχχουντσ ϕανε βαλικτ δδσϕηασδδη σδηφγ ασκϕηλκ τεχηνιχαλ αλαν ϕουν διξ τεχηνιχαλ ϕοην µαριανι

Areas and Lengths in Polar Coordinates

ITU-R BT ITU-R BT ( ) ITU-T J.61 (

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

Οδηγίες Εγγραφής στις Εξετάσεις για Ανεξάρτητους Υποψηφίους

Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat

A 1 A 2 A 3 B 1 B 2 B 3

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Chapter 6 BLM Answers

Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1

Outline Analog Communications. Lecture 05 Angle Modulation. Instantaneous Frequency and Frequency Deviation. Angle Modulation. Pierluigi SALVO ROSSI

και τα οφέλη για τον τομέα ανάπτυξης γης και οικοδομών

Η ΕΡΕΥΝΑ ΤΗΣ ΓΛΩΣΣΙΚΗΣ ΑΛΛΑΓΗΣ ΣΤΑ ΚΕΙΜΕΝΑ ΤΗΣ ΜΕΣΑΙΩΝΙΚΗΣ ΕΛΛΗΝΙΚΗΣ: ΜΕΘΟΔΟΛΟΓΙΚΗ ΔΙΕΡΕΥΝΗΣΗ ΤΩΝ

HW 3 Solutions 1. a) I use the auto.arima R function to search over models using AIC and decide on an ARMA(3,1)

Graded Refractive-Index

Ο νοσηλευτικός ρόλος στην πρόληψη του μελανώματος

Multi-GPU numerical simulation of electromagnetic waves

Consommation marchande et contraintes non monétaires au Canada ( )

Galatia SIL Keyboard Information

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

ΕΘΝΙΚΟ ΚΑΠΟ ΙΣΤΡΙΑΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΑΘΗΝΩΝ Ι ΡΥΜΑ ΝΟΜΙΚΩΝ ΟΙΚΟΝΟΜΙΚΩΝ ΠΟΛΙΤΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΓΡΑΠΤΗ ΕΡΓΑΣΙΑ ΣΤΟ ΣΥΝΤΑΓΜΑΤΙΚΟ ΙΚΑΙΟ

UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS General Certificate of Education Ordinary Level

MathDebate Οδηγός για τον χρήστη

Περίπτωση ασθενούς µε ιδιαίτερα ανθεκτική υπέρταση επιτυχώς αντιµετωπισθείσα µε απονεύρωση νεφρικών αρτηριών

Working Paper Series 06/2007. Regulating financial conglomerates. Freixas, X., Loranth, G. and Morrison, A.D.

Ferrite Chip Beads For Automotive Use

Η ΠΡΟΣΩΠΙΚΗ ΟΡΙΟΘΕΤΗΣΗ ΤΟΥ ΧΩΡΟΥ Η ΠΕΡΙΠΤΩΣΗ ΤΩΝ CHAT ROOMS

Διερεύνηση ακουστικών ιδιοτήτων Νεκρομαντείου Αχέροντα

Aluminum Electrolytic Capacitors (Large Can Type)

Assignment 1 Solutions Complex Sinusoids

Aluminum Electrolytic Capacitors

Math221: HW# 1 solutions

( ) Sine wave travelling to the right side

Global energy use: Decoupling or convergence?

ΔΓΡΑ JEAN MONNET «ΝΔΔ ΓΙΑΣΑΔΙ ΣΙ ΔΤΡΩΠΑΪΚΔ ΝΟΜΙΚΔ ΠΟΤΓΔ» ημειώζεις Δσρωπαϊκού Γικαίοσ και Δσρωπαϊκής Ολοκλήρωζης

(Biomass utilization for electric energy production)


RSA3408A 23 W-CDMA

PARTIAL NOTES for 6.1 Trigonometric Identities

Defects in Hard-Sphere Colloidal Crystals

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

38BXCS STANDARD RACK MODEL. DCS Input/Output Relay Card Series MODEL & SUFFIX CODE SELECTION 38BXCS INSTALLATION ORDERING INFORMATION RELATED PRODUCTS

Example Sheet 3 Solutions


Εφαρµογή του κανονισµού ECE 111 στο βέλτιστο σχεδιασµό βυτιοφόρου οχήµατος µεταφοράς υγρών καυσίµων

ACI sécurité informatique KAA (Key Authentification Ambient)

Transcript:

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 2 2 = 4 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 9 9 14.5mm 14.5mm 16 145 (1, 1), (1, 2),,(9, 9) (1, 1) (5, 6) Δt = (5, 6) (5, 5) (4, 5) (4, 4) s 1 (t) s 2 (t) s 3 (t) s 4 (t) (5, 6) (5, 5) (4, 5) (4, 4).81λ λ 9 9.41λ xz 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal z [mm] 6 4 2 2 4 6 Ch3 Ch4 Ch1 Ch2 5 5 x [mm] T =1/T (t)dt s (DC) i s (raw) i s 1 (t) s 2 (t) s 3 (t) s 4 (t) s i (t) =s (raw) i (t) s (DC) i (i =1, 2, 3, 4) s (raw) i (t) s (DC) i P BF (θ, φ) P BF (θ, φ) = 1 T T a(θ, φ) H s(t) 2 dt, = a(θ, φ) H R ss a(θ, φ). s(t) = [s 1 (t),s 2 (t),s 3 (t),s 4 (t)] T R ss R ss = 1 T s(t)s H (t)dt, T a(θ, φ) a(θ, φ) =[k r 1, k r 2, k r 3, k r 4 ] T, k r 1 r 2 r 3 r 4 k θ φ k(θ, φ) =k[sin θ cos φ, sin θ sin φ, cos θ] T, k = 2π/λ λ = 3.6 y(t) =w1s 1 (t) +w2s 2 (t) +w3s 3 (t) +w4s 4 (t) =w H s(t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal w =[w 1,w 2,w 3,w 4 ] T y(t) 2 = w H s(t) 2 = w H s(t)(w H s(t)) H = w H s(t)s H (t)w, E[ y(t) 2 ] = w H R ss w E[] R ss =E[s(t)s H (t)] s(t) P C (θ, φ) P C (θ, φ) =minw w H R ss w, subject to w H a(θ, φ) =1. w E[ y(t) 2 ]=w H R ss w (θ, φ) (θ, φ) (θ, φ) E[ y(t) 2 ] w P C (θ, φ) P C (θ, φ) = 1 a H (θ, φ)(r ss + ɛi) 1 a(θ, φ), I ɛ ɛ = ɛ tr(r ss ) P C (θ, φ) θ φ (θ,φ ) w opt =argminw w H R ss w, subject to w H a =1, w a a = a(θ,φ ) θ φ arg max θ,φ P C (θ, φ) L L(w,λ ) = 1 2 wh R ss w +Re[λ (w H a 1)] = 1 2 wh R ss w + 1 2 λ (w H a 1) + 1 2 λ (w T a 1), λ L(w,λ ) w wl(w,λ )=R ss w + λ a =. w w = λ R 1 ss a, R ss 1 λ =. a H R 1 ss a w = R 1 ss a. a H R 1 ss a w R ss R ss Rss 1 w opt = (R ss + ɛ I) 1 a a H (R ss + ɛ I) 1 a. s DCMP (t) s DCMP (t) =w H opts(t). ɛ = ɛ tr(r ss ) ɛ w H s(t) s d (t) (θ,φ ) s i (t) (θ i,φ i ) G(θ,φ )=1 G(θ i,φ i )= α(w) 2 w α(w) (θ i,φ i ) w H s(t) =s d (t) +α(w)s i (t) E[ s d (t)+α(w)s i (t) 2 ]=E[ s d (t) 2 ]+ α(w) 2 E[ s i (t) 2 ] s d (t) 2 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal w α(w) s i (t) s DCMP (t) (θ,φ ) s DCMP (t) s DCMP (t) xz (x, y) =(.3m,.5m) (x, y) = (.3m,.5m) s A (t) s B (t) s A (t)+s B (t) s A (t) s B (t) λ = 35.7 λ λ 62.7 123.9 xz y =.5 s A (t)+s B (t) ɛ =1 5 (x, z) =(28.9cm,.8cm) (θ,φ ) a s B (t) 1 j 1 j 1 +j 1+j s B (t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal [db] 5 5 z [cm] 5 1 15 2 25 1 1 5 5 1 3 x [cm] [db] 5 5 5 [db] 5 z [cm] 5 1 15 2 z [cm] 5 1 15 2 1 1 5 5 1 x [cm] 25 3 1 1 5 5 1 x [cm] 25 3 R ss s B (t) R ss w opt a P DCMP (θ, φ) =w H opta(θ, φ) ɛ =.1 z [cm] 5 5 1 1 5 5 1 x [cm] [db] s DCMP (t) =w H opts B (t) P r(t) 4 P 5 1 15 2 25 3 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 2 1 Imaginary 1 1 Ch3 Ch1 Ch4 Ch2 2 2 1 1 2 Real Imaginary.5 -.5-1 -1 -.5.5 1 Real s B (t) [db] s DCMP (t) z [cm] 5 5 1 1 5 5 1 x [cm] r s 1 (t) s DCMP (t) d DCMP (t) d DCMP (t) = λ 4π unwrap( s DCMP (t)), unwrap( ) θ(t) ( θ(t) θ(t Δt) π), unwrap(θ(t)) = θ(t)+2π (θ(t) θ(t Δt) < π), θ(t) 2π (θ(t) θ(t Δt) >π). Δt 2 2 4 6 8 1 Displacement [mm] 3 2 1 1 2 3 4 5 6 1 2 3 4 5 d DCMP (t) s DCMP (t) s B (t) d 1 (t) s 1 (t) d DCMP (t) s DCMP (t) s A (t)+s B (t) s 1 (t) s A (t)+s B (t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal [db] 2 2 5 1 Imaginary 1 Ch3 Ch1 Ch4 Ch2 2 2 1 1 2 Real z [cm] 5 1 1 5 5 1 x [cm] 2 4 6 8 1 s A (t)+s B (t) Displacement [mm] 1 2 3 4 5 6 7 8 1 2 3 4 5 Imaginary 1.5 -.5-1 -1 -.5.5 1 Real s 1 (t) s DCMP s A (t)+s B (t) R ss θ φ s DCMP (t) s A (t)+s B (t) t =1 Displacement [mm] 3 2 1 1 2 3 4 5 6 1 2 3 4 5 d DCMP (t) s DCMP (t) s A (t)+s B (t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 3 3 2 2 Displacement [µm] 1 1 Displacement [µm] 1 1 2 2 3 1 2 3 4 5 s DCMP (t) s B (t) 3 1 2 3 4 5 s 1 (t) s A (t)+s B (t) 15 s t 45 s μ t Displacement [µm] 3 2 1 1 2 3 1 2 3 4 5 s DCMP (t) s A (t)+s B (t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal s B (t) s 1 (t) s DCMP (t) Interbeat Interval [s].7.65.6.55.5 1 2 3 4 5 s B (t) Interbeat Interval [s].7.65.6.55.5 1 2 3 4 5 s A (t) +s B (t) 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal.7 12 Interbeat Interval [s].65.6.55 Heart Rate [bpm] 11 1 9.5 1 2 3 4 5 s A (t)+ s B (t) 8 1 2 3 4 5 Time [sec] s B (t).7 12 Interbeat Interval [s].65.6.55 Heart Rate [bpm] 11 1 9.5 1 2 3 4 5 s A (t) + s B (t) 8 1 2 3 4 5 Time [sec] s A (t) +s B (t) R s Δt τn ECG τn radar n =1, 2,,N Δt =.5 τn ECG τn radar < τ τ = 5 N R s = N /N R s R s 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal Heart Rate [bpm] 12 11 1 9 8 1 2 3 4 5 Time [sec] s A (t)+s B (t) Normalized Frequency.5.4.3.2.1 DCMP for One Participant DCMP for Two Participants Single Channel for Two Participants -2-1 1 2 Heart Rate Error [bpm] 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See

This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Citation information: DOI 1.119/JETCAS.218.289582, IEEE Journal 2156-3357 (c) 218 IEEE. Translations and content mining are permitted for academic research only. Personal use is also permitted, but republication/redistribution requires IEEE permission. See