ess cryogenic system process design...invited presentation c1ore-01 given at cec-icmc 2015, tucson,...

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ESS Cryogenic System Process Design Philipp Arnold Section Leader Cryogenics www.europeanspallationsource.se CEC – ICMC 2015 June 29, 2015 IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

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Page 1: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

ESS Cryogenic System Process Design

Philipp Arnold Section Leader Cryogenics

www.europeanspallationsource.se CEC – ICMC 2015

June 29, 2015

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 2: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

View of the Southwest in 2025

2

MAX IV

ESS

• Max IV – a national research facility, under construction, opens up in 2016 • Science City – a new part of town

Lund (113 500)

Malmö (309 000)

Copenhagen (1 200 000)

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Science city just outside Lund to become a new cluster in material science. MAX IV = electron synchrotron, ESS = neutron source complimentary applied research.
Page 3: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Cryogenics at ESS

Coldbox building Compressor building

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
- 600 m Linac, half cryogenic, to provide a 5 MW proton pulse 14 times per second. Rotating tungsten target with two cold moderators cooled with supercritical 17K hydrogen. Neutron instrument halls, comprising consumers of smaller quantities of LHe and LN2.
Page 4: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

4

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 5: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Pure Helium Gas Storage 1

20 m3 LHe Tank

Standalone Helium Purifier

Helium Recovery System

Pure Helium Gas Storage 2

Accelerator Cryoplant

Test & Instrument Cryoplant

5 m3 LHe Tank

Target Moderator Cryoplant

LHe Mobile Dewars

Test Stand Distribution

System

Instruments & Experiments

LN2 Storage Tanks

LN2 Mobile Dewars

Cryogenic Distribution

System

Cryomodules Cryomodule Test Stand

Target Distribution

System

Hydrogen Circulation Box

Hydrogen Moderator

5

(1) System overview

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
ACCP: 3kW @ 2K, 11kW @ 40K, 270 l/h Liquefaction special plant, power consumption in MW range, big industrial compressors, sophisticated CC system. TICP: 76W @ 2K, 420W @ 40K, 6 l/h Liquefaction plant well in the standard range. TMCP: 32kW @ 15-20K very large again, some challenges but not terribly sophisticated process, compared to ACCP. Large and sophisticated cryo-distribution system for all plants and their consumers.
Page 6: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

6

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 7: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.1) The Accelerator cryogenic setup

7

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 8: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.1) The Accelerator cryogenic setup

8

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Nice visualisation of some CMs and CDS. 3 types of CMs at ESS high beta and medium beta elliptical CMs and Spoke CMs.
Page 9: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.2) Cryomodule cooling at 2K

9

Production of 2 K helium in 2 K heat exchanger and a sub-sequent Joule-Thomson valve in each of the cryomodule–valve box assemblies

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
CM cooling with 2K and shield at about 40K, no 5K shield, no LN2. Heat load on CDS only on 4.5K, not 2K helium. independent warm-up / maintenance / cool-down of single cryomodules while the rest of the system is maintained in cold condition. One VBX per CM, all welded jumper connection. Vacuum barrier separating CM vacuum from CDS.
Page 10: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.3) The Accelerator cryoplant dutyspec

10

Type

Temperature range

Max. load Stage 1

Max. load Stage 2

Static and dynamic load in CMs

2 K 1850 W 2230 W

Recuperators and CDS load

2 – 4 K 630 W 830 W

Thermal shields

33 – 53 K 8 550 W 11 380 W

Coupler cooling

4.5 – 300 K 6.8 g/s 9.0 g/s

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
When CMs perform as expected only stage 1 loads apply. When CMs Q is insufficient then more of them need to be installed in contingency space. Everything already prepared, plant can easily be upgraded to stage 2 design.
Page 11: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.4) The Accelerator cryogenic load

11

0

500

1000

1500

2000

2500

3000

3500

0 10 20 30 40 50 60

ACCP

2K

heat

load

, W

Number of Cryomodules

ACCP 2K heat load vs number of installed CMs

Beam ON w/ safety factors

Beam ON w/o safety factors

Beam OFF w/ safety factors

Beam OFF w/o safety factors

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Several facts can be read out of this figure for 2K load which is representative for other ACCP loads as well. 1) load depends strongly on number of installed CMs. 2) substantial load contribution from static load, i.e. also when beam off. 3) quite big operation range also due to uncertainties. 4) it is possible that stage 2 is never required, either because CMs are so good or because not all safety margin is required.
Page 12: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(2.5) The Accelerator cryoplant process

12

300 K

115 K

70 K 53 K 33 K

24 K

9 K

6 K

4.5 K

Compressor skids with 3 identical screws

6 turbo expanders

Thermal shield ~43K

Connection to 20 m3 tank

3 cold turbo compressors

VFD for SPMP and LPMP

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Identical screws give space savings, advantages in spares concept and even possibilities to to spare each other. VFDs for SP and LP machines not only used for turndown but also for stage 2. T1/2 basically for liquefaction load and HX inefficiencies. T3 for shield. T4-6 for main load coming from CCs. Flow parts of TUs and CCs can be exchanged for stage 2.
Page 13: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

13

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 14: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

14 14

Proton beam window Moderator and reflector plugs

Target wheel

Neutron beam windows

Neutron beam extraction

(3.1) The Target Monolith

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Proton beam hits tungsten target wheel 14 times per second. Target wheel has 36 segments one pulse per segment gives rotation speed of 23.3 1/min. Majority of beam energy (5 MW) removed by helium cooling of the target wheel.
Page 15: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

15

(3.2) The Target Monolith inside

Target wheel

Proton beam window Moderator and reflector plugs

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Target has 42 neutron beam windows around the cold moderators, actually even more because of top and bottom moderator. 60 neutrons are produced per proton but only 1 out of 100T is reaching going through the neutron guides. Protons come with almost speed of light. Spallated neutrons have ~6.5% speed of light. To short wavelength for most of the instruments.
Page 16: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

16

Target wheel

Bottom MR plug

Proton beam

Top MR plug

(3.3) Moderator-Reflector system

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Moderated in water first and in cold hydrogen second neutrons cooled down to ~220 m/s (less than speed of sound). Quite complicated design. Supercritical hydrogen loop and general talk about target moderator cryoplant separated talk by JJ Tuesday 16:45.
Page 17: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(3.4) The Target cryogenic load

17

0

5

10

15

20

25

30

35

0 1 2 3 4 5 6

TMCP

hea

t loa

d, k

W

Beam power, MW

TMCP 15-20K heat load vs. beam power

Load w/ safety factors

Load w/o safety factors

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
The previous slides only to give background for the heat load on the cryogenic system. Hydrogen loop transfers helium to a helium loop where the heat has ultimately to be removed. Unlike ACCP only small portion static load, most of the load directly proportional to the beam power. Impressive load range to be covered by the TMCP.
Page 18: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(3.5) The Target Moderator cryoplant process (proposed by ESS)

18

300 K

90…120 K

60…80 K

23 K

20 K

15K

Helium buffers with “low” and “high” pressure region

Turbine for HXs

2 screw compressor skids

Intermediate “heating” of feed flow upstream turbines

Helium

20.5 K

17.0 K

Hydrogen

2 expansion turbines

Multi purpose ambient heater

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Large heat load, small dT high m*. Return temp upper limit by H2 loop. Feed temp lower limit by H2 solidification point. For reasonable pressure ratio of TUs: intermediate heating in HX4.
Page 19: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

19

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 20: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(4.1) Where sits the helium

1) ACCP: Over 2000 kg in Cryomodules and distribution system

20

0

500

1000

1500

2000

2500

NO CD

Helium mass in CMs & CDS w/o shield[kg]

VapourHelium

LiquidHelium

2) TMCP: Over 350 kg in Cryotransferline between helium and hydrogen box

3) TICP: About 600 kg in open loop system for neutron instruments

2 x 335 m x 4”

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Liquid @ 2K is 20% denser than at 4.4K but vapor at 4K is 25 times denser than @ 2K large impact of VLP line. CTL between He CBx Building and Target Building is 335 m per way, DN100 inner diameter. Open loop: means the 5000 l LHe storage tank 80% full, half of anticipated mobile dewars full, half of recovery full.
Page 21: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(4.2) Helium storage

1) Pure medium pressure tanks – 19 x 67 m3

– Theoretically up to 3.5 tons – Pressure restrictions for TICP and TMCP – Effectively ~ 3 tons

21

2) Liquid helium storage tank – 20 m3

– When filled to 80% another 2 tons – Used as ”2nd fill” and help in transient modes

(cool-down, pump-down)

3) Impure high pressure tanks or bundles

– 12 m3

– Nearly 300 kg – Used as buffer in recovery system

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
TICP run with normal Kaeser compressor, so ~12 bar would be maximal buffer pressure; with unit size of 67 m3 more than sufficient even for CM test. TMCP pressure restriction to the low limit: when system cold and full operation, LP maybe at 5 bar buffer pressure not <6 bar; plus 1 extra LP tank. HP storage takes roughly half Dewar.
Page 22: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

22

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 23: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(5.1) Definitions

23

Kinetic Experiments

Flux Integrated Experiments

A reliability of at least 90% should be provided for the duration of the measurement. The measurement will be considered failed when the beam power is reduced to less than 50% of the scheduled power for more than 1/10th of the measurement length.

For the duration of the experiment at least 90% of the experiments should have at least 85% of beam availability and on average more than 80% of the scheduled beam power. The beam will be considered unavailable when its power is less than 50% of its scheduled power for more than one minute.

At least 90% of the users should receive a neutron beam that will allow them to execute the full scope of their experiments

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
High level goal: “At least 90% of the users should receive a neutron beam that will allow them to execute the full scope of their experiments”. Kinetic: ~10% of all experiments continuous beam important for the entire measurement which is rather short (sec-min). Flux integrated: ~90% of all experiments beam interruptions acceptable but high integrated neutron flux important (1-7 days).
Page 24: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(5.2) Anticipated failure rates

24

Downtime duration Accelerator Target ICS SI

1 second - 6 seconds 120 per day - - -

6 seconds - 1 minute 40 per day - - -

1 minute - 6 minutes 4.8 per day - 40 per year -

6 minutes - 20 minutes 1.7 per day - 10 per year -

20 minutes - 1 hour 90 per year 2 per year 4 per year 3 per year

1 hour - 3 hours 29 per year 1 per year 2 per year 1 every 2 years

3 hours - 8 hours 15 per year 1 every 2 years 1 every 2 years 1 every 2 years

8 hours - 1 day 5.5 per year 1 every 2 years 1 every 5 years 1 every 3 years

1 day - 3 days 2.3 per year 1 every 2 years - 1 every 10 years

3 days - 10 days 1 every 5 years 1 every 20 years - -

more than 10 days 3 every 40 years 1 every 40 years - -

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 25: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(5.3) Backup compressor system

25

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Separate Bulk ORS for BC enables seamless switchover from HP to BC during operation. No VFD for BC but LP requires VFD in St2 SP to LP, LP to BC. Further measures to increase availability include. Double turbines and compressors for TMCP. 2nd fill helium storage (20 m3 tank). Connection of UPS backed TICP compressor to ACCP LP string to recover helium at long power outage.
Page 26: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Outline

1) System Overview

2) Accelerator Load and its Cryoplant

3) Target Moderator Load and its Cryoplant

4) Helium Management and Storage

5) Reliability and Availability

6) Energy

26

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 27: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(6.1) Energy high level goals

27

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
High level goal: build a sustainable facility. Renewable is not my job but for Responsible and Recyclable Cryogenics can do a lot.
Page 28: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(6.2) Heat recovery

28

• No elevated oil or helium temperatures out of compressor suppliers specs

• More efficient heat exchangers, especially oil coolers

• Dedicated cooling water circuit for cryoplant

• Cooling function has priority over heat recovery

Motor

Middle temperature

Supply

Oil separator

Helium compressor

Helium cooler

Oil cooler

Helium

High temperature

Return

Middle temperature

Return

25°C

30°C

27°C

40°C

73°C

32°C

32°C 65°C

37°C

70°C

Oil pump

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Presenter
Presentation Notes
Clean up with rumors from last ICEC – no, we don’t intend to destroy our compressors right after first start-up, crack oil, reduce lifetime etc. Quite straight-forward approach. Small dT on warm end side of the coolers with PFHX instead tube/shell HX. Closed secondary loop with own pumps.
Page 29: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

(6.3) Energy efficiency and sustainability

29

• Focus on process design and optimization

• Good match between plant and load by staging, dual equipment, VFDs for low pressure machines

• Focus on turn-down scenarios

• Incentive OPEX approach in ACCP and TMCP tender evaluation and contracts as well

• As much as possible helium recovery

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.

Page 30: ESS Cryogenic System Process Design...Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 July 2, 2015. View of the Southwest in 2025 2 MAX IV ESS • Max IV

Conclusions

30

• The conceptual design of the cryogenic system at ESS is finished

• One cryoplant is ordered, one out for quote, one to 90% specified ESS is rolling

• High level goals in terms of energy efficiency and sustainability can be met

• Continued work on meeting reliability and availability requirements

IEEE/CSC & ESAS SUPERCONDUCTIVITY NEWS FORUM (global edition), July 2015. Invited presentation C1OrE-01 given at CEC-ICMC 2015, Tucson, USA, June 28 – July 2, 2015.