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Study of an improved beam screen design for MKIs Study of an improved beam screen design for MKIs

Study of an improved beam screen design for MKIs - PowerPoint Presentation

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Study of an improved beam screen design for MKIs - PPT Presentation

Vasilis Vlachodimitropoulos Acknowledgements Mike Barnes Lorena Vega Cid 30052017 1 HLLHC WP14 Coordination Meeting Motivation 1 MKI overview given by Mike Circulating beam passes through Ushaped yokes ID: 793708

beam lhc wp14 coordination lhc beam coordination wp14 2017 meeting screen power rings mki ferrite impedance measurements run design

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Slide1

Study of an improved beam screen design for MKIs

Vasilis VlachodimitropoulosAcknowledgements: Mike Barnes, Lorena Vega Cid

30/05/2017

1

HL-LHC WP14 Coordination Meeting

Slide2

Motivation (1)

MKI overview given by Mike

Circulating beam passes through U-shaped yokes

Beam-ferrite interaction → ferrites heat up → if above Tc

we cannot safely inject → wait to cool down → long turn around times → PROBLEM!

Solution: e/m shield the beam from the yoke (= beam screen)

Ferrite

Screen

Curie Temperature

Above the Curie Temperature the ferrite temporarily looses its permeability.

Courtesy: Lorena Vega

30/05/2017

2

HL-LHC WP14 Coordination Meeting

Slide3

Motivation (2)

Beam screen upgraded during LS1 and as a result reduction of measured temperatures was observed

Observations during Run 2 are in agreement with predictions of existing models (see upcoming talk by Lorena)

Current MKI beam screen design is sufficient for Run 2

operation:

no heating issue is foreseen until the end of the run

E/m and thermal simulations predict that some yokes will exceed their Tc for HL-LHC beams

Further upgrades in the MKI beam screen design are necessary for HL-LHC!

30/05/2017

3

HL-LHC WP14 Coordination Meeting

Slide4

The present MKI beam screen

24 conductive wires inside a ceramic tube

Fast rise time: wires grounded at one end (downstream) and

capacitively coupled to the other (upstream)

Arrangement and extra vacuum gap to deal with HV issues

2 sets of 9 ferrite rings to damp low frequency modes

Note: overlapping region between screen conductors and grounded metallic cylinder

30/05/2017

4

HL-LHC WP14 Coordination Meeting

Slide5

Heating Process

Beam spectrum couples to real part of longitudinal impedance

R{Z

L}:

For MKI, Z

L

is now essentially geometric: overlapping region acts as

λ/2 cavity →

Beam looses energy primarily at the cavity’s resonant frequencies

Non uniform power distribution: ferrites (rings and yokes) close to the cavity are affected significantly more

30/05/2017

5

HL-LHC WP14 Coordination Meeting

Courtesy: Mike Barnes

Slide6

Solution we are looking into

Reduce overlap → upshift resonant frequencies to where the beam spectrum is reduced

Power loss estimates: depend on relative position of impedance peaks to beam harmonics

If overlap is reduced too much

beam screen is no longer effective: losses increase rapidly

Shorter cylinder + rings in the same position

→ part of power is dissipated in the rings before it reaches the yoke

30/05/2017

6

HL-LHC WP14 Coordination Meeting

Slide7

New proposal for overlap

Mechanical constraints: 81mm-long cylinder

→ 56mm overlap

Ferrite rings are interchanged: 4B3 ↔ 4M2

Kapton

layer to support the last 5 upstream ferrite rings – temporary solution for measurements

C

oncentrate on power loss estimatesExpected temperatures will be presented by Lorena

30/05/2017

7

HL-LHC WP14 Coordination Meeting

L

overlap

Exposed ferrite rings

Slide8

Comparison 1: Impedance Simulations

Power Loss

(W)

Post-LS1

56mm

Run 2

37/27/9722/15/16

HL-LHC135/97/35079/54/58

Nominal

Beam Parameters

ppb (e+11)Nbt

b (ns)Run 21.15

28081HL-LHC

2.227481

30/05/2017

8

HL-LHC WP14 Coordination Meeting†

PL was estimated in three ways:Directly from simulations (e.g. 380MHz for

post-LS1 design)With the first impedance peak at the frequency given by measurements (e.g. 420MHz)

With the first impedance peak at the lowest beam harmonic closest to the frequency given by measurements (e.g. 380MHz→ 400MHz)

Slide9

Comparison 2: Impedance Measurements

Transmission wire method and resonant method

30/05/2017

9

HL-LHC WP14 Coordination Meeting

Slide10

Comparison 3: Power

Distribution Simulations

% of total power

Post LS1

56mm

Upstream rings

43

90First 6 yokes23

4Most affected ring

927Most affected yoke8

1

Assume

HL-LHC: 120/80 Watt

+

Scaling factor: 4

Power (W)

Post LS156mm

Upstream rings205290

First 6 yokes11213

Most affected ring43

86Most affected yoke38.6

330/05/2017

10

HL-LHC WP14 Coordination Meeting

Slide11

Comparison 4: Power Distribution Measurements

Preliminary results

Probes at rings and yoke to measure received signal

Need to be repeated with probes in better locations

30/05/2017

11

HL-LHC WP14 Coordination Meeting

Slide12

Summary

Upgrade of the MKI beam screen is necessary for HL-LHC

An easily implemented design was presented

Power loss reduction & redistribution to easier to cool areas

Preliminary measurements seem to verify expected behaviour

New beam screen design to be implemented in MKI prototype and tested with Run 2 beams:

provided ongoing thermal studies

ensure

that no heating issue is expected!30/05/2017

12

HL-LHC WP14 Coordination Meeting

Slide13

Thank you for your attention!

30/05/2017

13

HL-LHC WP14 Coordination Meeting

Slide14

Questions?

Please, don’t ask me how hot we will get!

Lorena will come to that in a moment!

30/05/2017

14

HL-LHC WP14 Coordination Meeting