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APS-U FORUM MEETING THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN BEAMLINE JONATHAN KNOPP Mechanical Engineer Beamline Instrumentation XIANBO SHI Physicist June 14, 2018

THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

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Page 1: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

APS-U FORUM MEETING

THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN BEAMLINE

JONATHAN KNOPPMechanical EngineerBeamline Instrumentation

XIANBO SHIPhysicist

June 14, 2018

Page 2: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

APS-U FEATURE BEAMLINESUndulator WB mirror Monochromator

3Dnano 2.1 m planar 2.7 or 2.8 Yes, H DCM, H or V

Atomic 2.1 m revolver 2.5/2.1 Yes, H DCM/DMM, H

CHEX Cant (1.2 m SCU 1.85, 1.65) no Diamond SBM, DCM

CSSI 4.6 m revolver 2.5/2.1, or planar 2.7 Yes, H DCM&DMM

HEXM (1.75 m SCU1.65) X2 no Bent DLM, H

ISN 4.6 m revolver 2.5/2.1 Yes, V, two DCM/DMM

Polar (1.8 m SCAPE SCU 3.1) X2 no DCM, H

Ptycho 4.6 m revolver 2.5/2.1 Yes, H DCM, H

XPCS 4.6 m revolver 2.5/2.1 or HGVPU 2.7 Yes, H, two DCM/DMM, H

Page 3: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

IN-SITU NANOPROBEAPS-U FEATURE BEAMLINE

The In-Situ nanoprobe (ISN) beamline delivers highest-resolution imaging, spectroscopy, and tomography of energy materials and energy devices, as well as of other complex, hierarchical systems under in-situ and operando conditions.

The ISN beamline will provide a spot size as small as 20 nm using reflective optics.

Approximately 220 m long

Currently planned to be located at Sector 19.

5 – 30 keV

Two Mirrors as first optics for Harmonic Rejection and bouncing back the beam. Will focus to a BDA.

Page 4: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

The thermal bump on both M1 and M2 can be corrected by bending M2. Due tothe near 1:1 demagnification, bending M2 to a spherical cylinder is sufficient.The angle of M2 will need to be changed by small amounts accordingly tocompensate for the vertical displacement.

The heat load absorbed in M1 and M2 was calculated using SRCalc for Sicoated mirrors. The insertion device, 25 mm period and 4.6 m long, was tunedto different energies (5-12 keV).

CORRECTING FOR THERMAL BUMP

Page 5: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

ISN BEAMLINE U25/U21 revolver

M1 M2

Absorbedpower

Deformation

5 keV

-200

-100

0

100

200

Mirr

or L

engt

h (m

m)

-0.4 -0.2 0.0 0.2 0.4Mirror Width (mm)

Mirror 1, SiW/mm2

0.8

0.6

0.4

0.2

0.0 -200

-100

0

100

200

Mirr

or L

engt

h (m

m)

-0.4 -0.2 0.0 0.2 0.4Mirror Width (mm)

Mirror 2, Si W/mm2

0.025

0.020

0.015

0.010

0.005

0.000

-3.0

-2.0

-1.0

0.0

Def

orm

atio

n (μ

m)

-200 -100 0 100 200Mirror length (mm)

SE = 19 μrad

-0.06

-0.04

-0.02

0.00

Def

orm

atio

n (μ

m)

-200 -100 0 100 200Mirror length (mm)

SE = 0.38 μrad

Page 6: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

Photon energy 5 keV 6 keV 7 keV 8 keV 9 keV 10 keV 11 keV 12 keV

Ky for undulator U25 1.862 1.599 1.381 1.191 1.019 0.857 0.697 0.528

Total power absorbed by M1 (W) 429 329 260 190 130 80.9 44.2 20.3

Total power absorbed by M2 (W) 10.6 7.58 9.06 6.96 6.23 5.85 5.73 5.79

Focal size at BDA without deformation (µm), FWHM 16.6 15.4 14.4 13.6 13.0 12.5 12.0 11.6

M2 radius to focus at BDA without deformation (km) 11.0

Focal size at BDA with deformation1 (µm), FWHM 1129 809 589 398 257 155 84 47

Virtual source position relative to BDA2 (m) -39.9 -47.6 -60.3 -113.9 156.1 32.8 12.1 5.6

Corrected M2 radius (km) 4.38 5.10 5.72 6.57 7.51 8.49 9.4 10.1

M2 angle correction (degree) -1.4E-05 -1.1E-05 -9.0E-06 -7.0E-06 -5.0E-06 -3.0E-06 -5.0E-07 -1.1E-06

Corrected focal size at BDA (µm), FWHM 16.8 15.4 14.2 13.6 13.0 12.5 12.2 11.6

1M2 radius fixed at 11.0 km2Positive means downstream

Table 1. Result summary for fixed energy operation

The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical cylinder is sufficient.

Page 7: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

Photon energy 5 keV 5.1 keV (no correction on M2)

Ky for undulator U25 1.862 1.833

Total power absorbed by M1 (W) 429 418

Total power absorbed by M2 (W) 10.6 10.0

Focal size at BDA with R2 = 4.38 km optimized for 5 keV (µm), FWHM 16.8 21.0

Focal position relative to BDA (m) 0 -1.7

Table 2. Result summary for energy scan with undulator at 5 keV

• Scan energy by 100 eV at 5 keV will result in a focal size change from 17 µm to 21 µm at theBDA position. This will lead to some flux variation at the sample, but depends on the BDA size.

-40

-20

0

20

40

Ver

tical

pos

ition

(μm

)

-1000 -500 0 500 1000Horizontal position (μm)

-40

-20

0

20

40

Ver

tical

pos

ition

(μm

)

-1000 -500 0 500 1000Horizontal position (μm)

Page 8: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

The ray tracings below compare the ideal focus (left) with the image obtained when the deformation on M1 and M2 are included (middle). The figure on the right shows the focus when the radius of M2 as been decreased from the original

value (11.0 km) to the value calculated (4.38 km) from the virtual image created by the heat bumps. Note that the angle of M2 will need to be change by 0.24 µrad to compensate for the vertical

displacement

RAY-TRACING STUDY

-40

-20

0

20

40

Ver

tical

pos

ition

(μm

)

-1000 -500 0 500 1000Horizontal position (μm)

-1000

-500

0

500

1000

Ver

tical

pos

ition

(μm

)

-1000 -500 0 500 1000Horizontal position (μm)

-40

-20

0

20

40

Ver

tical

pos

ition

(μm

)

-1000 -500 0 500 1000Horizontal position (μm)

Plane M1Cylinder M2 (RM2 = 11.0 km)

With thermal bump on M1, M2

After bending correction of M2 to RM2 = 4.38 km

Page 9: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

COOLING SCHEMEInternal Cooling

InSync Internally Cooled Mirrors. No Longer Frit Bonded

Modeled a mirror based on their drawings

InSync provided metrology data showing the deformation due to internal pressure

Page 10: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

-3.0

-2.5

-2.0

-1.5

-1.0

-0.5

0.0

Def

orm

atio

n (μ

m)

-200 -100 0 100 200Mirror Length (mm)

-0.30

-0.25

-0.20

-0.15

-0.10

-0.05

0.00

Deformation at 5 keV Side cooled (19 μrad) Internally cooled (3.9 μrad)

COOLING SCHEME

-0.14

-0.12

-0.10

-0.08

-0.06

-0.04

-0.02

0.00

Def

orm

atio

n (μ

m)

-100 0 100Mirror Length (mm)

Deformation at 5 keVspherical term removed

Side cooled (0.14 μrad) Internally cooled (0.82 μrad)

-0.03

-0.02

-0.01

0.00

0.01

Def

orm

atio

n (μ

m)

-100 -50 0 50 100Mirror Length (mm)

Deformation at 5 keVspherical term removed

Side cooled (0.05 μrad) Internally cooled (0.16 μrad)

M1 deformation

Internal Cooling

Page 11: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

COOLING SCHEMESide Cooled with Notch

0.00E+00

5.00E-04

1.00E-03

1.50E-03

2.00E-03

2.50E-03

0 50 100 150 200 250 300 350 400

Def

orm

atio

n (m

m)

Mirror Length (mm)

Vertical Deformation at Various Notch Sizes

8 x 10 mm

8 x 5 mm

8 x 8 mm

8 x 8.5 mm

8 x 7.5 mm

* L. Zhang ESRF

Page 12: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

HIGH HEAT LOAD OPTICS WORKING GROUP

Discuss analysis and cooling schemes of Mirrors, Monos, Masks, Beamstops, etc.

Discuss best practices for cooling and mounting optics

Peter Eng will present next meeting on thermal considerations at Sector 13

NEXT MEETING JUNE 20th AT 2:00 P.M.– B4100

Jonathan Knopp and Xianbo Shi

Page 13: THERMAL ANALYSIS OF HIGH HEAT LOAD MIRRORS FOR ISN … · The thermal bump on both M1 and M2 can be corrected by bending M2. Due to the near 1:1 demagnification, bending M2 to a spherical

www.anl.gov

THANKS! QUESTIONS?