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TIME-RESOLVED SYNCHROTRON X-RAY COMPUTED TOMOGRAPHY AS A TOOL FOR GROUNDWATER REMEDIATION Nathaly Lopes Archilha 1 Gabriel Schubert Costa 1 , Tannaz Pak 2 1 Brazilian Synchrotron Light Laboratory (LNLS/CNPEM) and 2 Teesside University [email protected]
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TIME-RESOLVED SYNCHROTRON X-RAY COMPUTED … › ... › t3_14-50-nathaly-lopes-archila.pdf · Nathaly Lopes Archilha1 Gabriel Schubert Costa1, Tannaz Pak2 1Brazilian Synchrotron

Jul 04, 2020

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Page 1: TIME-RESOLVED SYNCHROTRON X-RAY COMPUTED … › ... › t3_14-50-nathaly-lopes-archila.pdf · Nathaly Lopes Archilha1 Gabriel Schubert Costa1, Tannaz Pak2 1Brazilian Synchrotron

TIME-RESOLVED SYNCHROTRON X-RAY COMPUTED

TOMOGRAPHY AS A TOOL FOR GROUNDWATER

REMEDIATION

Nathaly Lopes Archilha1

Gabriel Schubert Costa1, Tannaz Pak2

1Brazilian Synchrotron Light Laboratory (LNLS/CNPEM) and 2Teesside University

[email protected]

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Agenda

- The Brazilian Center for Research in Energy and Materials (CNPEM)

- The Brazilian Synchrotron Light Source and the Sirius Project

- Time resolved X-ray tomography

- Application for Groundwater remediation: in-situ reaction between

TCE and nZVI

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National Laboratory - Free for academic users- Partnership with private company

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Relativistic Model

Cone emission

P. Willmot Introduction to Synchrotron Radiation Science

1

𝜸= 1 − Τ𝒗2 𝒄2 ~ 10−3 deg

The Brazilian Synchrotron Light Sourcea particle accelerator

Classic Model

Isotropic emission

Centripetal acceleration

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Wavelength?

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And what is the impact?

http://www.chemistryland.com/CHM107/Final/FinalWritten.html

NEAR IR VISIBLE UV X-RAYRADIO WAVE

MICROWAVE SHORTWAVE IR

LONGWAVE IR

Higher energy, smaller wavelength

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Incident photon

Sample

Photoemission Fluorescence

Transmission

ElasticScattering

InelasticScattering

Electromagnetic Radiation

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The Sirius Project

Ago, 2018

3 GeV, 250 pm rad

IPÊ

(AP-RIXS/AP-XPS)

90 eV - 1600 eVCARNAÚBA

(nanoprobe/ptychography)

2 -15 keV

MOGNO

(Cone beam CT)

30/90keV

Short period undula t or

Long per iod undulat or

3 .2T Superb end

SABIÁ

(ARPES/XMCD)

90 eV - 1600 eV

MANACÁ

(micro and nano MX)5 - 20 keV

CATERETÊ

(pw-CDI/XPCS)

3- 15 keV

HARPIA

(TR-XPD)

5 - 24 keV

IMBÚIA

(IR-SNOM)

0.001 - 1 eV

HERA

(XTMS)

40-120 keV

SAGUI

(SAXS)

4-24 keV

XARU

(EXAFS)

4- 45 keV

3 - 35 keV

EMA

(Extreme Conditions)

COLIBRI

(CDI/PEEM)

90 eV - 1600 eV

Large Microscope: most interesting/challenging materials, with nanometricresolution and several contrast mechanisms

Experimental ProgramsTender nano-probe for spectro-ptychography; Large FOV (40 mm) coherent diffraction imaging; Bragg CDI/XRD/XAFS under extreme conditions; Serial micro and nano MX; Tender x-ray RIXS; Time resolved powder diffraction; High-throughput SAXSARPES/XMCD; AP-RIXS/XPS; CDI/PEEMCone beam high energy tomography; EXAFS; High energy X-Ray diffraction; Nano-FTIR

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X-ray computed tomography

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Mogno Beamline @SiriusCone beam x-ray imaging

Energy Range ˜20, 40 and 70 keV

Resolution ˜ 100 nm to 55mm

Field of View up to 85 mm (zoom-in)

Contrast Electron density, phase contrast

Dose Very efficient

Speed Fast (~1 mCTs/s)

Equivalent to parallel beam with:

Magnification:

1.5” rock and soil samples

A 3D image in 1 second

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~1 mm ~20 mm

Applications – zoom tomographyfrom hundreds of nm to dozens of micrometers

- Zoom tomography: reveal unresolved connections between pores

- Truly non destructive scans (cone beam)

- No special sample preparation required

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Application: time-resolved XCT

More extreme conditions

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Application: In-situ degradation of TCE using nZVI nanoparticles

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Application: In-situ degradation of TCE using nZVI nanoparticles