Chromospheric and Transition Region dynamics

Size: px
Start display at page:

Download "Chromospheric and Transition Region dynamics"

Transcription

1 Chromospheric and Transition Region dynamics Luc Rouppe van der Voort University of Oslo

2

3

4

5

6

7 IRIS: type II spicules are heated to at least TR temperatures Pereira et al ApJL 792

8 type II spicules are heated to at least TR temperatures IRIS Mg II 2796 Å SDO/AIA He II 304 Å Hinode Ca II H IRIS Si IV 1400 Å Quiet Sun at South Pole sample of 54 spicules: 41 (76%) fade in Ca H 30 (56%) brighten in Si IV when Ca H fades Skogsrud et al ApJ in press (arxiv ), see poster Skogsrud et al.

9 Ca II H Mg II 2796 Å Si IV 1400 Å He II 304 Å sample of 54 spicules: 41 (76%) fade in Ca H 30 (56%) brighten in Si IV when Ca H fades 24 (44%) are brighter in Si IV at top Skogsrud et al ApJ in press (arxiv ), see poster Skogsrud et al.

10 SST/CRISP: Hα -54 km/s, μ= Mm On-disk we observe absorption features with same characteristics as off-limb type II spicules

11 Rapid Blue-shifted Excursions (RBE) time λ average profile λ Hα -60 km/s Rouppe van der Voort et al ApJ 705 RBEs are the disk-counterparts of type II spicules

12 RRE (Rapid Red-shifted Excursion) RBE (Rapid Blue-shifted Excursion) Ca II km/s Ca II 8542 Ca II 8542 ±16 km/s Hα Doppler Disk center Quiet Sun Sekse et al ApJ 769

13 RRE (Rapid Red-shifted Excursion) RBE (Rapid Blue-shifted Excursion) Ca II km/s Ca II kinds of motion: upflow swaying torsion Ca II 8542 ±16 km/s Hα Doppler Disk center Quiet Sun Sekse et al ApJ 769

14 Transition Region response to type II spicules on-disk: network jets (see Tian et al Science)

15 Transition Region response to type II spicules on-disk: network jets (see Tian et al Science) RRE RBE

16 IRIS network jets (see Tian et al. Science 2014) IRIS SJI 1330 IRIS SJI 1400 RRE RBE SST Halpha Doppler ±46 km/s SST Halpha -46 km/s De Pontieu et al Science, Rouppe van der Voort et al ApJL 799

17 IRIS SJI 1330 IRIS SJI 1400 RRE RBE SST Halpha Doppler ±46 km/s SST Halpha -46 km/s De Pontieu et al Science, Rouppe van der Voort et al ApJL 799

18 Connection network jets and RBE/RREs RRE RBE torsional motion and associated heating De Pontieu et al Science, Rouppe van der Voort et al ApJL 799

19 Connection network jets and RBE/RREs Rouppe van der Voort et al ApJL 799

20 RBE: Rapid Blue-shifted Excursion Rouppe van der Voort et al ApJL 799

21 RRE: Rapid Red-shifted Excursion Rouppe van der Voort et al ApJL

22 Ca II H Mg II 2796 Å Si IV 1400 Å He II 304 Å parabolic trajectory for type II in Ca H? (33%) Note: heating along the spicule length and higher velocities Skogsrud et al ApJ in press (arxiv ), see poster Skogsrud et al.

23 Type I Type II parabolic trajectory for type II in Ca H? Note: heating along the spicule length and higher velocities Skogsrud et al ApJ in press (arxiv ), see poster Skogsrud et al.

24 Active region plage: dynamic fibrils (type I spicules)

25 Active region plage: dynamic fibrils (type I spicules)

26 Active region plage: dynamic fibrils (type I spicules) SST 04-Oct-2005 Hansteen et al. 2006, De Pontieu et al. 2007

27 Active region plage: dynamic fibrils (type I spicules) SST 04-Oct-2005 Hansteen et al. 2006, De Pontieu et al. 2007

28 Active region plage: dynamic fibrils (type I spicules) Hansteen et al. 2006, De Pontieu et al. 2007

29 Active region plage: dynamic fibrils (type I spicules) Radiative MHD simulations show the formation of dynamic chromospheric features similar to DFs, driven by shocks caused by upward propagating waves in the chromosphere. Hansteen et al. 2006, De Pontieu et al. 2007

30 observations vs simulations: x-t plots observations simulations Spicule-like features in simulations show parabolic paths similar to those observed in Dynamic Fibrils. Hansteen et al. 2006, De Pontieu et al. 2007

31 Active region plage: dynamic fibrils (type I spicules)

32 Active region plage: dynamic fibrils (type I spicules)

33 Hα line center Si IV 1400

34 Active region plage: dynamic fibrils (type I spicules) Hα vs. Si IV 1400

35 Active region plage: dynamic fibrils (type I spicules) Hα line center Ca II 8542 line center Hα line center Ca II 8542 line center Si IV 1400 Å Mg II 2796 Å Si IV 1400 Å Mg II 2796 Å Hα -18 km/s Hα +18 km/s Hα -18 km/s Hα +18 km/s

36 Active region plage: dynamic fibrils (type I spicules) Ca II 8542 Å Hα 6563 Å Mg II k 2796 Å Si IV 1403 Å Transition Region response to dynamic fibrils: Si IV brightening, blueshift and line broadening

37 caution when comparing spectra extended structures

38 Active region plage: dynamic fibrils (type I spicules) large spatial raster Si IV SJI 1400 Si IV 1403 intensity Si IV 1403 Doppler ±20 km/s Si IV 1403 width 8-15 km/s Transition Region response to dynamic fibrils: Si IV brightening, blueshift and line broadening

39 Transition region response of internetwork acoustic grains? Martinez-Sykora et al ApJ 803

40 Transition region response of internetwork acoustic grains? mostly continuum emission from 55Å bandpass filters Martinez-Sykora et al ApJ 803

41 Conclusions Clear Transition Region response in spicules: type II: heating along the spicule length type I / dynamic fibrils: only at top Internetwork acoustic grains: (very) weak response in TR lines, IRIS SJI 1400 & 1330 emission mostly continuum

Heating diagnostics with MHD waves

Heating diagnostics with MHD waves Heating diagnostics with MHD waves R. Erdélyi & Y. Taroyan Robertus@sheffield.ac.uk SP 2 RC, Department of Applied Mathematics, The University of Sheffield (UK) The solar corona 1860s coronium discovered

More information

EIF-OIF-IIF-IRG-ERG Final Activity and Management Report

EIF-OIF-IIF-IRG-ERG Final Activity and Management Report EUROPEAN COMMISSION RESEARCH DG HUMAN RESOURCES AND MOBILITY EIF-OIF-IIF-IRG-ERG Final Activity and Management Report Project Acronym: SoND Project Full Name: Solar Network Dynamics Marie Curie Actions

More information

CHROMOSPHERIC AND TRANSITION REGION INTERNETWORK OSCILLATIONS: A SIGNATURE OF UPWARD-PROPAGATING WAVES AND

CHROMOSPHERIC AND TRANSITION REGION INTERNETWORK OSCILLATIONS: A SIGNATURE OF UPWARD-PROPAGATING WAVES AND THE ASTROPHYSICAL JOURNAL, 531:1150È1160, 2000 March 10 ( 2000. The American Astronomical Society. All rights reserved. Printed in U.S.A. CHROMOSPHERIC AND TRANSITION REGION INTERNETWORK OSCILLATIONS:

More information

3D MODEL ATMOSPHERES OF THE SUN AND LATE-TYPE STARS. Remo Collet Australian National University

3D MODEL ATMOSPHERES OF THE SUN AND LATE-TYPE STARS. Remo Collet Australian National University 3D MODEL ATMOSPHERES OF THE SUN AND LATE-TYPE STARS Remo Collet Australian National University STELLAR SPECTRA Stellar spectra carry the information about the physical properties and compositions of stars

More information

From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation?

From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation? From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation? From lowest energy to highest energy, which of the following correctly

More information

arxiv:1309.5213v1 [astro-ph.sr] 20 Sep 2013

arxiv:1309.5213v1 [astro-ph.sr] 20 Sep 2013 Draft version September 23, 2013 Preprint typeset using L A TEX style emulateapj v. 5/25/10 FIRST HIGH-RESOLUTION IMAGES OF THE SUN IN THE 2796 Å Mg II k LINE T. L. Riethmüller, 1 S. K. Solanki, 1,2 J.

More information

I. Introduction. II. Review

I. Introduction. II. Review I. Introduction Seismic Emission from Solar Flares C. Lindsey NorthWest Research Associates Colorado Research Associates Division A.-C. Donea, D. Besliu-Ionescu, H. Moradi and P. S. Cally Centre from Stellar

More information

The Doppler Effect & Hubble

The Doppler Effect & Hubble The Doppler Effect & Hubble Objectives Explain the Doppler Effect. Describe Hubble s discoveries. Explain Hubble s Law. The Doppler Effect The Doppler Effect is named after Austrian physicist Christian

More information

# % # & ( ) +,.& / 0 / # 1 ) (123(4(.&&5 1!(3 21 6 + 4 13! ( 2

# % # & ( ) +,.& / 0 / # 1 ) (123(4(.&&5 1!(3 21 6 + 4 13! ( 2 ! # % # & ( +,.& / 0 / # 1 (123(4(.&&5 1!(3 21 6 + 4 13! ( 2 7 A&A 481, 247 252 (2008 DOI: 10.1051/0004-6361:20078610 c ESO 2008 Astronomy & Astrophysics Coronal loop oscillations and diagnostics with

More information

High resolution images obtained with Solar Optical Telescope on Hinode. SOLAR-B Project Office National Astronomical Observatory of Japan (NAOJ)

High resolution images obtained with Solar Optical Telescope on Hinode. SOLAR-B Project Office National Astronomical Observatory of Japan (NAOJ) High resolution images obtained with Solar Optical Telescope on Hinode SOLAR-B Project Office National Astronomical Observatory of Japan (NAOJ) Temperature stratification of solar atmosphere G-band Ca

More information

Non-radial pulsations (NRP) or co-rotating photospheric Helium clouds in ζ Tau?

Non-radial pulsations (NRP) or co-rotating photospheric Helium clouds in ζ Tau? Non-radial pulsations (NRP) or co-rotating photospheric Helium clouds in ζ Tau? Description of the phenomenon Investigations of the HeI6678 line profile in ζ Tau show that it is quite different from a

More information

PERIODIC SPECTRAL LINE ASYMMETRIES IN SOLAR CORONAL STRUCTURES FROM SLOW MAGNETOACOUSTIC WAVES

PERIODIC SPECTRAL LINE ASYMMETRIES IN SOLAR CORONAL STRUCTURES FROM SLOW MAGNETOACOUSTIC WAVES DRAFT VERSION SEPTEMBER 17 010 Preprint typeset using L A TEX style emulateapj v. 08//09 PERIODIC SPECTRAL LINE ASYMMETRIES IN SOLAR CORONAL STRUCTURES FROM SLOW MAGNETOACOUSTIC WAVES E. VERWICHTE Centre

More information

8.1 Radio Emission from Solar System objects

8.1 Radio Emission from Solar System objects 8.1 Radio Emission from Solar System objects 8.1.1 Moon and Terrestrial planets At visible wavelengths all the emission seen from these objects is due to light reflected from the sun. However at radio

More information

Solar Ast ro p h y s ics

Solar Ast ro p h y s ics Peter V. Foukal Solar Ast ro p h y s ics Second, Revised Edition WI LEY- VCH WILEY-VCH Verlag Co. KCaA Contents Preface 1 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2 2.1 2.1.1 2.1.2 2.2 2.2.1 2.2.2 2.2.3 2.3

More information

Howard Eskildsen often uploads some of his wonderful and exquisite solar

Howard Eskildsen often uploads some of his wonderful and exquisite solar Solar Images Taken with Calcium K-Line Filters Howard L. Cohen January 2014 (Rev. March 2015) Howard Eskildsen s beautiful images of the Sun uploaded to the AAC website may appear strange and unfamiliar

More information

Coronal Heating Problem

Coronal Heating Problem Mani Chandra Arnab Dhabal Raziman T V PHY690C Course Project Indian Institute of Technology Kanpur Outline 1 2 3 Source of the energy Mechanism of energy dissipation Proposed mechanisms Regions of the

More information

Rest optical spectroscopy of FeLoBALs and LoBALs at intermediate redshift

Rest optical spectroscopy of FeLoBALs and LoBALs at intermediate redshift Rest optical spectroscopy of FeLoBALs and LoBALs at intermediate redshift Kentaro Aoki Subaru Telescope, National Astronomical Observatory of Japan E-mail: kaoki@subaru.naoj.org NLS1s and low-ionization

More information

Solar Flares and the Chromosphere

Solar Flares and the Chromosphere Solar Flares and the Chromosphere A white paper for the Decadal Survey * L. Fletcher, R. Turkmani, H. S. Hudson, S. L. Hawley, A. Kowalski, A. Berlicki, P. Heinzel Background: The solar chromosphere is

More information

Francesco Piacentini. Title. Page 1

Francesco Piacentini. Title. Page 1 Page 1 Page 2 Layers core -- nuclear burning central part of the Sun radiative zone -- the layer below convection zone where energy is transported by photons convection zone -- layer of the Sun just below

More information

Solar Active Region:Heating and Dynamics L.K. Harra-Murnion and S.A. Matthews Mullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking, Surrey RH5 6NT, U.K. H. Hara and K.

More information

Spectral Line II. G ij (t) are calibrated as in chapter 5. To calibrated B ij (ν), observe a bright source that is known to be spectrally flat

Spectral Line II. G ij (t) are calibrated as in chapter 5. To calibrated B ij (ν), observe a bright source that is known to be spectrally flat Spectral Line II: Calibration and Analysis 2 Spectral Line II John Hibbard Bandpass Calibration Flagging Continuum Subtraction Imaging Visualization Analysis Reference: Michael Rupen, Chapter 11 Synthesis

More information

Kinetic physics of the solar wind

Kinetic physics of the solar wind "What science do we need to do in the next six years to prepare for Solar Orbiter and Solar Probe Plus?" Kinetic physics of the solar wind Eckart Marsch Max-Planck-Institut für Sonnensystemforschung Complementary

More information

Be Stars. By Carla Morton

Be Stars. By Carla Morton Be Stars By Carla Morton Index 1. Stars 2. Spectral types 3. B Stars 4. Be stars 5. Bibliography How stars are formed Stars are composed of gas Hydrogen is the main component of stars. Stars are formed

More information

Active noise control in practice: transformer station

Active noise control in practice: transformer station Active noise control in practice: transformer station Edwin Buikema 1 ; Fokke D. van der Ploeg 2 ; Jan H. Granneman 3 1, 2, 3 Peutz bv, Netherlands ABSTRACT Based on literature and extensive measurements

More information

Heating & Cooling in Molecular Clouds

Heating & Cooling in Molecular Clouds Lecture 8: Cloud Stability Heating & Cooling in Molecular Clouds Balance of heating and cooling processes helps to set the temperature in the gas. This then sets the minimum internal pressure in a core

More information

Wave-particle and wave-wave interactions in the Solar Wind: simulations and observations

Wave-particle and wave-wave interactions in the Solar Wind: simulations and observations Wave-particle and wave-wave interactions in the Solar Wind: simulations and observations Lorenzo Matteini University of Florence, Italy In collaboration with Petr Hellinger, Simone Landi, and Marco Velli

More information

THE SIMULATION OF MOVING SOUND SOURCES. John M. Chowning

THE SIMULATION OF MOVING SOUND SOURCES. John M. Chowning THE SIMULATION OF MOVING SOUND SOURCES John M. Chowning The Center for Computer Research in Music and Acoustics (CCRMA) Department of Music Stanford University, Stanford, CA 94306 jmc165@home.com (first

More information

Solar Irradiance Variability Observed During Solar Cycle 23

Solar Irradiance Variability Observed During Solar Cycle 23 Solar Irradiance Variability Observed During Solar Cycle 23 Introduction Solar Cycle Results for Climate Change Solar Cycle Results for Space Weather Tom Woods LASP / University

More information

http://www.guido.be/intranet/enqueteoverview/tabid/152/ctl/eresults...

http://www.guido.be/intranet/enqueteoverview/tabid/152/ctl/eresults... 1 van 70 20/03/2014 11:55 EnqueteDescription 2 van 70 20/03/2014 11:55 3 van 70 20/03/2014 11:55 4 van 70 20/03/2014 11:55 5 van 70 20/03/2014 11:55 6 van 70 20/03/2014 11:55 7 van 70 20/03/2014 11:55

More information

Solar Wind Heating by MHD Turbulence

Solar Wind Heating by MHD Turbulence Solar Wind Heating by MHD Turbulence C. S. Ng, A. Bhattacharjee, and D. Munsi Space Science Center University of New Hampshire Acknowledgment: P. A. Isenberg Work partially supported by NSF, NASA CMSO

More information

Association of Mid-Infrared Solar Plages With Calcium K Line Emissions and Magnetic Structures

Association of Mid-Infrared Solar Plages With Calcium K Line Emissions and Magnetic Structures Association of Mid-Infrared Solar Plages With Calcium K Line Emissions and Magnetic Structures R.MARCON 1 Institute of Physics Gleb Watagin, State University of Campinas, Campinas, Brazil P.KAUFMANN 2,3,

More information

Solar atmosphere. Solar activity and solar wind. Reading for this week: Chap. 6.2, 6.3, 6.5, 6.7 Homework #2 (posted on website) due Oct.

Solar atmosphere. Solar activity and solar wind. Reading for this week: Chap. 6.2, 6.3, 6.5, 6.7 Homework #2 (posted on website) due Oct. Solar activity and solar wind Solar atmosphere Reading for this week: Chap. 6.2, 6.3, 6.5, 6.7 Homework #2 (posted on website) due Oct. 17 Photosphere - visible surface of sun. Only ~100 km thick. Features

More information

Cosmic Structure Formation and Dynamics: Cosmological N-body Simulations of Galaxy Formation and Magnetohydrodynamic Simulations of Solar Atmosphere

Cosmic Structure Formation and Dynamics: Cosmological N-body Simulations of Galaxy Formation and Magnetohydrodynamic Simulations of Solar Atmosphere Chapter 3 Epoch Making Simulation Cosmic Structure Formation and Dynamics: Cosmological N-body Simulations of Galaxy Formation and Magnetohydrodynamic Simulations of Solar Atmosphere Project Representative

More information

Solar System science with the IRAM interferometer. Recent Solar System science with the IRAM Plateau de Bure interferometer

Solar System science with the IRAM interferometer. Recent Solar System science with the IRAM Plateau de Bure interferometer Recent Solar System science with the IRAM Plateau de Bure interferometer J. Boissier (Institut de radioastronomie millimétrique) Contact: boissier@iram.fr Outline Planet moons Io Titan Planets Mars Comets

More information

SSO Transmission Grating Spectrograph (TGS) User s Guide

SSO Transmission Grating Spectrograph (TGS) User s Guide SSO Transmission Grating Spectrograph (TGS) User s Guide The Rigel TGS User s Guide available online explains how a transmission grating spectrograph (TGS) works and how efficient they are. Please refer

More information

The CGM around Dwarf Galaxies

The CGM around Dwarf Galaxies The CGM around Dwarf Galaxies Rongmon Bordoloi STScI + the COS-Halos Team What is the CGM? Shen et al. 212 jectedcolumndensityinacubeof5(proper)kpc Diffuse gas, including metals and dust, o2en on extending

More information

Fundamentals of Acoustics & Practical HVAC Design Considerations. Demir Doken Acoustic Engineer

Fundamentals of Acoustics & Practical HVAC Design Considerations. Demir Doken Acoustic Engineer Fundamentals of Acoustics & Practical HVAC Design Considerations Demir Doken Acoustic Engineer What is sound? Sound is a mechanical wave that is an oscillation of pressure transmitted through some medium

More information

- thus, the total number of atoms per second that absorb a photon is

- thus, the total number of atoms per second that absorb a photon is Stimulated Emission of Radiation - stimulated emission is referring to the emission of radiation (a photon) from one quantum system at its transition frequency induced by the presence of other photons

More information

Astro 102 Test 5 Review Spring 2016. See Old Test 4 #16-23, Test 5 #1-3, Old Final #1-14

Astro 102 Test 5 Review Spring 2016. See Old Test 4 #16-23, Test 5 #1-3, Old Final #1-14 Astro 102 Test 5 Review Spring 2016 See Old Test 4 #16-23, Test 5 #1-3, Old Final #1-14 Sec 14.5 Expanding Universe Know: Doppler shift, redshift, Hubble s Law, cosmic distance ladder, standard candles,

More information

Principles of Medical Ultrasound. Pai-Chi Li Department of Electrical Engineering National Taiwan University

Principles of Medical Ultrasound. Pai-Chi Li Department of Electrical Engineering National Taiwan University Principles of Medical Ultrasound Pai-Chi Li Department of Electrical Engineering National Taiwan University What is Medical Ultrasound? Prevention: actions taken to avoid diseases. Diagnosis: the process

More information

Coronal expansion and solar wind

Coronal expansion and solar wind Coronal expansion and solar wind The solar corona over the solar cycle Coronal and interplanetary temperatures Coronal expansion and solar wind acceleration Origin of solar wind in magnetic network Multi-fluid

More information

Astro 301/ Fall 2005 (48310) Introduction to Astronomy

Astro 301/ Fall 2005 (48310) Introduction to Astronomy Astro 301/ Fall 2005 (48310) Introduction to Astronomy Instructor: Professor Shardha Jogee TAs: David Fisher, Donghui Jeong, and Miranda Nordhaus Lecture 22 = Tu Nov 15 Lecture 23 = Th Nov 17 http://www.as.utexas.edu/~sj/a301-fa05/

More information

Warning : HαT telescope must NOT be used for solar observation without additional filters. This is the user responsibility to check that his filter

Warning : HαT telescope must NOT be used for solar observation without additional filters. This is the user responsibility to check that his filter For high resolution chromosphere observation and imaging in Hα band Warning : HαT telescope must NOT be used for solar observation without additional filters. This is the user responsibility to check that

More information

CHROMOSPHERIC DYNAMICS FROM RHESSI AND RESIK DATA

CHROMOSPHERIC DYNAMICS FROM RHESSI AND RESIK DATA CHROMOSPHERIC DYNAMICS FROM RHESSI AND RESIK DATA T. Mrozek 1,2, S. Kołomański 2,B. Sylwester 1, A. Kępa 1, J. Sylwester 1, S. Gburek 1, M. Siarkowski 1, M. Gryciuk 1, M. Stęślicki 1 1 Solar Physics Division,

More information

Evidence in White Light of Post-CME Current Sheets Mostly Observational

Evidence in White Light of Post-CME Current Sheets Mostly Observational Evidence in White Light of Post-CME Current Sheets Mostly Observational David Webb ISR, Boston College OUTLINE Review previous results of SMM & LASCO WL rays trailing CMEs - Lifetimes, lengths (heights)

More information

APPLICATION NOTE AP050830

APPLICATION NOTE AP050830 APPLICATION NOTE AP050830 Selection and use of Ultrasonic Ceramic Transducers Pro-Wave Electronics Corp. E-mail: sales@pro-wave.com.tw URL: http://www.prowave.com.tw The purpose of this application note

More information

Searching for young proto-planetary disks from ALMA archival data Final presentation

Searching for young proto-planetary disks from ALMA archival data Final presentation Searching for young proto-planetary disks from ALMA archival data Final presentation Speaker: Pou Ieng Cheong( 張 寶 瑩 ) 1 Supervisor: Shih Ping Lai( 賴 詩 萍 ) 2,3 1 Department of electrophysics, NCTU 2 Department

More information

J-PAS: low-resolution (R 50) spectroscopy over 8000 deg 2

J-PAS: low-resolution (R 50) spectroscopy over 8000 deg 2 J-PAS: low-resolution (R 50) spectroscopy over 8000 deg 2 C. López-Sanjuan J. Cenarro, L. A. Díaz-García, J. Varela, K. Viironen, & the J-PAS team Centro de Estudio de Física del Cosmos de Aragón 10th

More information

Universities of Leeds, Sheffield and York http://eprints.whiterose.ac.uk/

Universities of Leeds, Sheffield and York http://eprints.whiterose.ac.uk/ promoting access to White Rose research papers Universities of Leeds, Sheffield and York http://eprints.whiterose.ac.uk/ This is an author produced version of a paper published in Solar Physics. White

More information

Summer School Greenhouse Horticulture

Summer School Greenhouse Horticulture Programme Summer School Greenhouse Horticulture Wageningen University Campus Course leader: Date: 24 August 4 September 2015 Lecturers Dr Sjaak Bakker, General Manager, Wageningen University, Greenhouse

More information

5. The Nature of Light. Does Light Travel Infinitely Fast? EMR Travels At Finite Speed. EMR: Electric & Magnetic Waves

5. The Nature of Light. Does Light Travel Infinitely Fast? EMR Travels At Finite Speed. EMR: Electric & Magnetic Waves 5. The Nature of Light Light travels in vacuum at 3.0. 10 8 m/s Light is one form of electromagnetic radiation Continuous radiation: Based on temperature Wien s Law & the Stefan-Boltzmann Law Light has

More information

C3: LIMMCAST: Modelling of steel casting. Helmholtz-Zentrum Dresden-Rossendorf (HZDR), D-01314 Dresden 2

C3: LIMMCAST: Modelling of steel casting. Helmholtz-Zentrum Dresden-Rossendorf (HZDR), D-01314 Dresden 2 C3: LIMMCAST: Modelling of steel casting S. Eckert 1, R. Schwarze 2 1 Helmholtz-Zentrum Dresden-Rossendorf (HZDR), D-01314 Dresden 2 TU Bergakademie Freiberg, Inst. für Mechanik und Fluiddynamik, D-09599

More information

Neutron Stars. How were neutron stars discovered? The first neutron star was discovered by 24-year-old graduate student Jocelyn Bell in 1967.

Neutron Stars. How were neutron stars discovered? The first neutron star was discovered by 24-year-old graduate student Jocelyn Bell in 1967. Neutron Stars How were neutron stars discovered? The first neutron star was discovered by 24-year-old graduate student Jocelyn Bell in 1967. Using a radio telescope she noticed regular pulses of radio

More information

Modeling the Expanding Universe

Modeling the Expanding Universe H9 Modeling the Expanding Universe Activity H9 Grade Level: 8 12 Source: This activity is produced by the Universe Forum at NASA s Office of Space Science, along with their Structure and Evolution of the

More information

IRAS 11590 6452 in BHR 71 a binary protostellar system?

IRAS 11590 6452 in BHR 71 a binary protostellar system? 2001 June 10 ApJ, 554, 91L IRAS 11590 6452 in BHR 71 a binary protostellar system? Tyler L. Bourke Harvard-Smithsonian Center for Astrophysics, 60 Garden Street MS 42, Cambridge MA 02138, USA ABSTRACT

More information

Interaction of Energy and Matter Gravity Measurement: Using Doppler Shifts to Measure Mass Concentration TEACHER GUIDE

Interaction of Energy and Matter Gravity Measurement: Using Doppler Shifts to Measure Mass Concentration TEACHER GUIDE Interaction of Energy and Matter Gravity Measurement: Using Doppler Shifts to Measure Mass Concentration TEACHER GUIDE EMR and the Dawn Mission Electromagnetic radiation (EMR) will play a major role in

More information

ILLUSTRATIVE EXAMPLE: Given: A = 3 and B = 4 if we now want the value of C=? C = 3 + 4 = 9 + 16 = 25 or 2

ILLUSTRATIVE EXAMPLE: Given: A = 3 and B = 4 if we now want the value of C=? C = 3 + 4 = 9 + 16 = 25 or 2 Forensic Spectral Anaylysis: Warm up! The study of triangles has been done since ancient times. Many of the early discoveries about triangles are still used today. We will only be concerned with the "right

More information

Tribology and Mechanical Testing Unit

Tribology and Mechanical Testing Unit Pin Abrasion Testing Using the Micro-Tribometer mod. CETR-UMT 2 ASTM G132-96 Test method for determining the wear resistance of a pin of test material during sliding on an abrasive cloth, paper, or plastic

More information

Group Session 1-3 Rain and Cloud Observations

Group Session 1-3 Rain and Cloud Observations Group Session 1-3 Rain and Cloud Observations Targets in Science Plans CINDY Science Plan (Apr. 2009) DYNAMO SPO (Jul. 2009) Atmospheric Research a. Preconditioning processes b. Rossby wave c. Diabatic

More information

FRAUNHOFER INSTITUTE FOR INTEg RATEd CIRCUITS IIS. drm TesT equipment

FRAUNHOFER INSTITUTE FOR INTEg RATEd CIRCUITS IIS. drm TesT equipment FRAUNHOFER INSTITUTE FOR INTEg RATEd CIRCUITS IIS drm TesT equipment dt230 playback of drm signals recording of drm signals channel simulation receiver performance analysis real-time modulation Architecture

More information

Orbits of the Lennard-Jones Potential

Orbits of the Lennard-Jones Potential Orbits of the Lennard-Jones Potential Prashanth S. Venkataram July 28, 2012 1 Introduction The Lennard-Jones potential describes weak interactions between neutral atoms and molecules. Unlike the potentials

More information

Cosmic Dust in an Expanding Universe?

Cosmic Dust in an Expanding Universe? Planck energy - E - ev Cosmic Dust in an Expanding Universe? QED Radiations, Discovery Bay, Hong Kong, China nanoqed@gmail.com Copyright 2016 Horizon Research Publishing All rights reserved. Abstract Dust

More information

Presentation of problem T1 (9 points): The Maribo Meteorite

Presentation of problem T1 (9 points): The Maribo Meteorite Presentation of problem T1 (9 points): The Maribo Meteorite Definitions Meteoroid. A small particle (typically smaller than 1 m) from a comet or an asteroid. Meteorite: A meteoroid that impacts the ground

More information

165 points. Name Date Period. Column B a. Cepheid variables b. luminosity c. RR Lyrae variables d. Sagittarius e. variable stars

165 points. Name Date Period. Column B a. Cepheid variables b. luminosity c. RR Lyrae variables d. Sagittarius e. variable stars Name Date Period 30 GALAXIES AND THE UNIVERSE SECTION 30.1 The Milky Way Galaxy In your textbook, read about discovering the Milky Way. (20 points) For each item in Column A, write the letter of the matching

More information

The Unique, Optically-Dominated Quasar Jet of PKS 1421-490

The Unique, Optically-Dominated Quasar Jet of PKS 1421-490 The Unique, Optically-Dominated Quasar Jet of PKS 1421-490 J.M. Gelbord & H.L. Marshall (MIT) D.M. Worrall & M. Birkinshaw (U. Bristol) J.E.J. Lovell, R. Ojha, L. Godfrey & D.L. Jauncey (CSIRO) D.A. Schwartz

More information

Follow-up Observations of SPY White Dwarf + M-Dwarf Binaries

Follow-up Observations of SPY White Dwarf + M-Dwarf Binaries 15 th European Workshop on White Dwarfs ASP Conference Series, Vol. 372, 2007 R. Napiwotzki and M. R. Burleigh Follow-up Observations of SPY White Dwarf + M-Dwarf Binaries P. F. L. Maxted Astrophysics

More information

Widths of spectral lines

Widths of spectral lines Widths of spectral lines Real spectral lines are broadened because: Energy levels are not infinitely sharp. Atoms are moving relative to observer. 3 mechanisms determine profile φ(ν) Quantum mechanical

More information

Multiple Delay Coherence Imaging Charge Exchange Recombination Spectroscopy

Multiple Delay Coherence Imaging Charge Exchange Recombination Spectroscopy Multiple Delay Coherence Imaging Charge Exchange Recombination Spectroscopy Peter Urlings 9 th of October, 2015 A report submitted in fulfilment of the requirements of the degree of Master of Applied Physics

More information

ACOUSTICAL MODEL FOR HYBRID NVH SIMULATION OF ELECTRICAL VEHICLES

ACOUSTICAL MODEL FOR HYBRID NVH SIMULATION OF ELECTRICAL VEHICLES ACOUSTICAL MODEL FOR HYBRID NVH SIMULATION OF ELECTRICAL VEHICLES Johannes Klein, Gottfried Behler, Michael Vorländer Institute of Technical Acoustics, RWTH Aachen University, Kopernikusstr. 5, 52074 Aachen,

More information

Acoustic Terms, Definitions and General Information

Acoustic Terms, Definitions and General Information Acoustic Terms, Definitions and General Information Authored by: Daniel Ziobroski Acoustic Engineer Environmental and Acoustic Engineering GE Energy Charles Powers Program Manager Environmental and Acoustic

More information

Curriculum Overview IB Physics SL YEAR 1 JUNIOR TERM I (2011)

Curriculum Overview IB Physics SL YEAR 1 JUNIOR TERM I (2011) Curriculum Overview IB Physics SL YEAR 1 JUNIOR TERM I (2011) Resources: Gregg Kerr, Nancy Kerr, (2004) Physics International Baccalaureate, IBID Press, Victoria, Australia. Tim Kirk and Neil Hodgson Physics

More information

Lecture 14. Introduction to the Sun

Lecture 14. Introduction to the Sun Lecture 14 Introduction to the Sun ALMA discovers planets forming in a protoplanetary disc. Open Q: what physics do we learn about the Sun? 1. Energy - nuclear energy - magnetic energy 2. Radiation - continuum

More information

Pericenter passage of the gas cloud G2 in the Galactic Center

Pericenter passage of the gas cloud G2 in the Galactic Center Pericenter passage of the gas cloud G2 in the Galactic Center S Gillessen 1, R Genzel 1,2, T K Fritz 1, F Eisenhauer 1, O Pfuhl 1, T Ott 1, M Schartmann 4,1, A Ballone 4,1 and A Burkert 4,1 1 Max Planck

More information

3 - Atomic Absorption Spectroscopy

3 - Atomic Absorption Spectroscopy 3 - Atomic Absorption Spectroscopy Introduction Atomic-absorption (AA) spectroscopy uses the absorption of light to measure the concentration of gas-phase atoms. Since samples are usually liquids or solids,

More information

Cooperative multi-agents detection with spatially distributed array sensors

Cooperative multi-agents detection with spatially distributed array sensors Cooperative multi-agents detection with spatially distributed array sensors Belkacem BENADDA and Fethi Tarik BENDIMERAD Dept. of Electrical and Electronic Engineering, University of Abou Bekr Belkaid Tlemcen,

More information

Simulation at Aeronautics Test Facilities A University Perspective Helen L. Reed, Ph.D., P.E. ASEB meeting, Irvine CA 15 October 2014 1500-1640

Simulation at Aeronautics Test Facilities A University Perspective Helen L. Reed, Ph.D., P.E. ASEB meeting, Irvine CA 15 October 2014 1500-1640 Simulation at Aeronautics Test A University Perspective Helen L. Reed, Ph.D., P.E. ASEB meeting, Irvine CA 15 October 2014 1500-1640 Questions How has the ability to do increasingly accurate modeling and

More information

Solar Eruption - How to Understand It

Solar Eruption - How to Understand It Understanding solar eruptions: an observational perspective on space weather Karel Schrijver Lockheed Martin Advanced Technology Center Solar-C; 2013/11/11; Takayama, Japan Space weather user objectives:

More information

CFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER

CFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER International Journal of Advancements in Research & Technology, Volume 1, Issue2, July-2012 1 CFD SIMULATION OF SDHW STORAGE TANK WITH AND WITHOUT HEATER ABSTRACT (1) Mr. Mainak Bhaumik M.E. (Thermal Engg.)

More information

The Milky Way Galaxy is Heading for a Major Cosmic Collision

The Milky Way Galaxy is Heading for a Major Cosmic Collision The Milky Way Galaxy is Heading for a Major Cosmic Collision Roeland van der Marel (STScI) [based on work with a team of collaborators reported in the Astrophysical Journal July 2012] Hubble Science Briefing

More information

PHYSICS FOUNDATIONS SOCIETY THE DYNAMIC UNIVERSE TOWARD A UNIFIED PICTURE OF PHYSICAL REALITY TUOMO SUNTOLA

PHYSICS FOUNDATIONS SOCIETY THE DYNAMIC UNIVERSE TOWARD A UNIFIED PICTURE OF PHYSICAL REALITY TUOMO SUNTOLA PHYSICS FOUNDATIONS SOCIETY THE DYNAMIC UNIVERSE TOWARD A UNIFIED PICTURE OF PHYSICAL REALITY TUOMO SUNTOLA Published by PHYSICS FOUNDATIONS SOCIETY Espoo, Finland www.physicsfoundations.org Printed by

More information

Metal Abundances of Accretion Discs in AM CVn Binaries

Metal Abundances of Accretion Discs in AM CVn Binaries Metal Abundances of Accretion Discs in AM CVn Binaries Thorsten Nagel D.-J. Kusterer, T. Rauch, K. Werner Institut für Astronomie/Astrophysik Kepler Center for Astro and Particle Physics Universität Tübingen

More information

Testing thermo-acoustic sound generation in water with proton and laser beams

Testing thermo-acoustic sound generation in water with proton and laser beams International ARENA Workshop DESY, Zeuthen 17th 19th of May 25 Testing thermo-acoustic sound generation in water with proton and laser beams Kay Graf Universität Erlangen-Nürnberg Physikalisches Institut

More information

Intermediate-Mass Black Holes (IMBHs) in Globular Clusters? HST Proper Motion Constraints. Roeland van der Marel

Intermediate-Mass Black Holes (IMBHs) in Globular Clusters? HST Proper Motion Constraints. Roeland van der Marel Intermediate-Mass Black Holes (IMBHs) in Globular Clusters? HST Proper Motion Constraints Roeland van der Marel Why Study IMBHs in Globular Clusters (GCs)? IMBHs: IMBHs can probe a new BH mass range, between

More information

IMPROVED CCD DETECTORS FOR HIGH SPEED, CHARGE EXCHANGE SPECTROSCOPY STUDIES ON THE DIII D TOKAMAK

IMPROVED CCD DETECTORS FOR HIGH SPEED, CHARGE EXCHANGE SPECTROSCOPY STUDIES ON THE DIII D TOKAMAK IMPROVED CCD DETECTORS FOR HIGH SPEED, CHARGE EXCHANGE SPECTROSCOPY STUDIES ON THE TOKAMAK by K.H. Burrell P. Gohil, R.J. Groebner, D.H. Kaplan, D.G. Nilson,* J.I. Robinson, and D.M. Thomas General Atomics,

More information

Space Weather Forecasts for Civil Aviation & Spaceflight. Bill Murtagh NOAA Space Environment Center Boulder, Colorado

Space Weather Forecasts for Civil Aviation & Spaceflight. Bill Murtagh NOAA Space Environment Center Boulder, Colorado Space Weather Forecasts for Civil Aviation & Spaceflight Bill Murtagh NOAA Space Environment Center Boulder, Colorado Space Weather, Aviation, and Spaceflight: Opportunities for Space Weather Research

More information

Indiana's Academic Standards 2010 ICP Indiana's Academic Standards 2016 ICP. map) that describe the relationship acceleration, velocity and distance.

Indiana's Academic Standards 2010 ICP Indiana's Academic Standards 2016 ICP. map) that describe the relationship acceleration, velocity and distance. .1.1 Measure the motion of objects to understand.1.1 Develop graphical, the relationships among distance, velocity and mathematical, and pictorial acceleration. Develop deeper understanding through representations

More information

Blackbody Radiation References INTRODUCTION

Blackbody Radiation References INTRODUCTION Blackbody Radiation References 1) R.A. Serway, R.J. Beichner: Physics for Scientists and Engineers with Modern Physics, 5 th Edition, Vol. 2, Ch.40, Saunders College Publishing (A Division of Harcourt

More information

Modelling clumpy! galactic disks

Modelling clumpy! galactic disks Modelling clumpy! galactic disks Simone Bianchi INAF-Osservatorio Astrofisico di Arcetri, Firenze with TRADING! Transfer of RAdiation through Dust IN Galaxies (Bianchi 2008) Radiative Transfer models"

More information

AGN-driven winds and ionized clouds moving along the jet in PKS 0521-365

AGN-driven winds and ionized clouds moving along the jet in PKS 0521-365 GH 2015: Forming and Fueling Supermassive Black Hole Seeds July 6-24, 2015, Tonantzintla, Puebla AGN-driven winds and ionized clouds moving along the jet in PKS 0521-365 Eric Faustino Jiménez-Andrade ericja@inaoep.mx

More information

The sun and the solar corona

The sun and the solar corona The sun and the solar corona Introduction The Sun of our solar system is a typical star of intermediate size and luminosity. Its radius is about 696000 km, and it rotates with a period that increases with

More information

SIZE. Energy. Non-Mechanical Energy. Mechanical Energy. Part II. Examples of Non-Mechanical Energy. Examples of Mechanical Energy.

SIZE. Energy. Non-Mechanical Energy. Mechanical Energy. Part II. Examples of Non-Mechanical Energy. Examples of Mechanical Energy. Energy Part II Non-Mechanical Energy Wait a minute if all energy is either kinetic or potential and TME = KE + PE then how can there possibly be such thing as non-mechanical energy!?!? Mechanical Energy

More information

SphinX:A Fast Solar Photometer in X-rays. J. Sylwester 1,, S. Kuzin 2, Yu. D. Kotov 3, F. Farnik 4 & F. Reale 5

SphinX:A Fast Solar Photometer in X-rays. J. Sylwester 1,, S. Kuzin 2, Yu. D. Kotov 3, F. Farnik 4 & F. Reale 5 J. Astrophys. Astr. (2008) 29, 339 343 SphinX:A Fast Solar Photometer in X-rays J. Sylwester 1,, S. Kuzin 2, Yu. D. Kotov 3, F. Farnik 4 & F. Reale 5 1 Space Research Center, Polish Academy of Sciences,

More information

Antonio Rampoldi Struttura Complessa di Radiologia Interventistica Azienda Ospedale Niguarda Ca Granda, Milano. Terminology

Antonio Rampoldi Struttura Complessa di Radiologia Interventistica Azienda Ospedale Niguarda Ca Granda, Milano. Terminology Biophysical principles and clinical applications of MRgFUS Alberto Torresin Struttura Complessa di Fisica Sanitaria Azienda, Milano Università degli Studi di Milano Dip. di Fisica Antonio Rampoldi Struttura

More information

Gaia: Solar System observations

Gaia: Solar System observations Gaia: Solar System observations Paolo Tanga Observatoire de la Côte d Azur (France) Gaia will also observe Asteroids (~250.000 most known) Comets Mainly Main Belt Asteroids (MBA) Several NEOs Other populations

More information

SPACE WEATHER INTERPRETING THE WIND. Petra Vanlommel & Luciano Rodriguez

SPACE WEATHER INTERPRETING THE WIND. Petra Vanlommel & Luciano Rodriguez SPACE WEATHER INTERPRETING THE WIND Petra Vanlommel & Luciano Rodriguez THE SUN LOSES ENERGY Radiation Mass Particles THE SUN LOSES ENERGY PHYSICAL REPHRASING Total Solar Irradiance Solar Wind Fast Particles

More information

Light as a Wave. The Nature of Light. EM Radiation Spectrum. EM Radiation Spectrum. Electromagnetic Radiation

Light as a Wave. The Nature of Light. EM Radiation Spectrum. EM Radiation Spectrum. Electromagnetic Radiation The Nature of Light Light and other forms of radiation carry information to us from distance astronomical objects Visible light is a subset of a huge spectrum of electromagnetic radiation Maxwell pioneered

More information

Proton temperature and Plasma Volatility

Proton temperature and Plasma Volatility The microstate of the solar wind Radial gradients of kinetic temperatures Velocity distribution functions Ion composition and suprathermal electrons Coulomb collisions in the solar wind Waves and plasma

More information

General aviation & Business System Level Applications and Requirements Electrical Technologies for the Aviation of the Future Europe-Japan Symposium

General aviation & Business System Level Applications and Requirements Electrical Technologies for the Aviation of the Future Europe-Japan Symposium General aviation & Business System Level Applications and Requirements Electrical Technologies for the Aviation of the Future Europe-Japan Symposium 26 March 2015 2015 MITSUBISHI HEAVY INDUSTRIES, LTD.

More information

Amateur Solar Observing

Amateur Solar Observing Amateur Solar Observing - or - How not to fry your eyeball! Why observe the sun? No more late nights Light pollution? What s that? Ever-changing surface Impacts to society Just plain cool! Obligatory safety

More information