1 radiation safety aspects of the linear collider b. racky, a. leuschner, n. tesch radiation...

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1

Radiation Safety Aspects of Radiation Safety Aspects of the Linear Colliderthe Linear Collider

B. Racky, A. Leuschner, N. Tesch

Radiation Protection Group

TeV Superconducting Linear Accelerator

2

Radiation Safety Aspects of TESLARadiation Safety Aspects of TESLA

Overview TESLA

Locations of beam loss

Protection of the public

• exposure limits

• exposure paths

Protection of the staff

3

Top view , route on map

4

Some data of TESLA :Some data of TESLA :

5

Side view with earth cover

6

Main locations of beam lossMain locations of beam loss

7

Calculations of doses and activitiesCalculations of doses and activities

• MC code FLUKA99

• fluence/ dose conversion: ICRP

Neutron and Gamma fieldsNeutron and Gamma fields

Muon fieldsMuon fields

Activity concentrationsActivity concentrations

• MC code FLUKA99

(option resnuclei)

• analytical model

(1- dimenional transport)

8

Protection of the PublicProtection of the Public(local population and environment)(local population and environment)

• Stray radiation fields

• Radioactivity of released tunnel air

• Radioactivity of drinking water

• Activation of soil

9

Protection of the PublicProtection of the Public

Sum of all exposures

Release of radioactive air

Activation of groundwater

Activation of soil

1 mSv/a 0,1 mSv/a

0,3 mSv/a

0,3 mSv/a ?

?

0,03 mSv/a

0,03 mSv/a

< natural activity

10

Stray radiation fields due to neutrons

1,0E-07

1,0E-06

1,0E-05

1,0E-04

1,0E-03

1,0E-02

1,0E-01

1,0E+00

1,0E+01

1,0E+02

1,0E+03

1,0E+04

1,0E+05

1,0E+06

1,0E+07

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15

Thickness of the sand cover [m]

An

nu

al d

ose

[µS

v]

natural exposure

minimum cover average cover

intranuclear cascadeneutrons

giant resonanceneutrons

electromagnetic cascade photons

11

Stray radiation fields due to myons

12

Release of radioactive airRelease of radioactive air

Nuclide half life3 H 12 a

7 Be 53 d11 C 20 m14 C 6 ka13 N 10 m15 O 2 m38 Cl 27 m39 Cl 56 m37 Ar 35 d41 Ar 1.8 h

Produced Nuclei

Main air activation zone

in the tunnel, near IP:

100 kW beam loss

(collimators)

13

Release of radioactive airRelease of radioactive air

Radioactive air can be released

without any permission,

if the mean annual

activity concentration

is below given nuclide specific limits.

(leading to a dose < 0,3 mSv/a

for the worst case of exposure)

§§§§§

For a mixture of nuclei :

0.11

n

iCL

Ci

A

A

ratio < 0.1

14

Release of radioactive airRelease of radioactive air

Overview ventilation system S. II-251 TDR

Should it be operated as a closed or open system?

15

Release of radioactive airRelease of radioactive air

Open system :

Open system :

Tunnel ventilation rate : 0,8 m/s, 6*104 m3/h

length of collimator section : 100 m

volume of activation zone : 2000 m3

distance to exhaust station : 5 km

delay time : 1.4 h

Closed system :

Closed system :

data :data :

Ventilation switched off during 1 month operation,

air blown out on each monthly maintenance day

Ventilation switched on during operation,

air blown out permanently

16

Release of radioactive airRelease of radioactive air

Nuclide half lifelimit: Ac L

(Bq/m3)Ac max outlet

(Bq/m3)ann. Ac mean

(Bq/m3)ratio

Ac mean/ Ac L

3 H 12 a 5.0* 102 1.67* 103 4.61* 10-2 9.2* 10-5

7 Be 53 d 3.0* 103 1.27* 104 3.51* 10-1 1.2* 10-4

11 C 20 m 1.5* 104 4.29* 103 1.19* 10-1 7.9* 10-6

14 C 6 ka 4.0* 103 2.87* 102 7.96* 10-3 2.0* 10-6

13 N 10 m 1.0* 104 5.68* 102 1.57* 10-2 1.6* 10-6

15 O 2 m 5.0* 103 3.40* 10-8 9,43* 10-13 1.9* 10-16

38 Cl 27 m 2.5* 103 9.81* 102 2.72* 10-2 1.1* 10-5

39 Cl 56 m 3.0* 103 1.37* 103 3.80* 10-2 1.3* 10-5

37 Ar 35 d 1.0* 109 2.01* 109 5.58* 10-2 5.6* 10-11

41 Ar 1.8 h 1.0* 103 3.07* 103 8.51* 10-1 8.5* 10-4

Closed systemClosed system

Sum of all ratios = 0.0011 << 1.0 and << 0.1

17

Release of radioactive airRelease of radioactive air

Nuclide half lifelimit: Ac L

(Bq/m3)Ac max outlet

(Bq/m3)ann. Ac mean

(Bq/m3)ratio

Ac mean/ Ac L

3 H 12 a 5.0* 102 8.00* 10-2 4.57* 10-2 9.1* 10-5

7 Be 53 d 3.0* 103 7.37* 10-1 4.21* 10-1 1.4* 10-4

11 C 20 m 1.5* 104 3.04* 102 1.73* 102 1.2* 10-2

14 C 6 ka 4.0* 103 1.38* 10-2 7.90* 10-3 2.0* 10-6

13 N 10 m 1.0* 104 8.20* 101 4.67* 101 4.7* 10-3

15 O 2 m 5.0* 103 2.42* 10-8 1.38* 10-8 2.8* 10-12

38 Cl 27 m 2.5* 103 3.81* 101 2.17* 101 8.7* 10-3

39 Cl 56 m 3.0* 103 3.56* 101 2.04* 101 6.8* 10-3

37 Ar 35 d 1.0* 109 1.29* 10-1 7.34* 10-2 7.3* 10-11

41 Ar 1.8 h 1.0* 103 4.04* 102 2.31* 102 2.3* 10-1

Open systemOpen system

Sum of all ratios = 0.26 < 1.0 but > 0.1

18

Release of radioactive airRelease of radioactive air

Conclusions A closed ventilation system leads to much

smaller release of radioactivity

Also an open system would fulfill

the legal requirements

Compromise ?

open system with bypassed release stations closed to

loss points

19

Activation of soil and ground waterActivation of soil and ground water

wet soil (27% water)

concrete shielding (3 m)

in the vicinity of a main dump

dump

TESLA lumi run:TESLA lumi run:

Operation time: 5000 h (1 year)

Energy: 250 GeV

power: 12 MW

20

Activity concentration of wet soilActivity concentration of wet soil

Most relevant nuclei Sum of all activity concentrations:

Nuclide half life3 H 12 a

7 Be 53 d18 F 110 m

22 Na 2.6 a24 Na 15 h28 Mg 21 h

32 P 14 d33 P 25 d35 S 88 d

37 Ar 35 d42 K 12 h43 K 22 h48 V 16 d49 V 330 d

51 Cr 28 d54 Mn 312 d55 Fe 2.7 a

0

10

20

30

40

50

60

70

80

90

ring1 ring2 ring3 ring4 ring5

saturation values5000 h operation

Bq/g

rings of 50 cm thickness

21

Activation of Soil and GroundwaterActivation of Soil and Groundwaterregion of 50 cm around a main dump after 5000 h of

operation

sandsand waterwater

7 Be

7 Be

3 H

3 H

22 Na

Silicon 32 %

Oxygen 53 %

Aluminium 4 %

Oxygen 89 %

100 %

100 %

15 %

natural activity:

0.3 -1 Bq/g

Dose, consuming 800 l/a

2.5 mSv (?% 22Na)

3H : 2.60 Bq/g

22Na : 0.45 Bq/g

7Be : ? Bq/g

22Na : ? Bq/g

22

Transport of ground waterTransport of ground water

Ground water flow: (expert‘s report)

area north dump south dump

descent 1m / 750m 1m/ 900m

permeability 5* 10-5 m/s 5* 10-5 m/s

filter velocity 6.7* 10-8 m/s 5.6* 10-8 m/s

distance velocity 2.2* 10-7 m/s 1.9* 10-7 m/s

distance velocity 6.9 m/ year 6.0 m/ year

error about 80% ?

23

Transport of activated ground waterTransport of activated ground wateractivation zone: north dump 12 m

south dump 18 m

At what distance is the activity concentration

so low, that drinking 800 l /a results in a dose of 30 µSv/a ?

vd

edilfdcAdcA )

0()(

Distance calculations for the dominant nuclide Na-22

After activation:

24

Zones of activated ground waterZones of activated ground water Distance Ac for 30 µSv/a after

velocity distance time

(m/s) (m) (a)

5.0 * 10-6 42 0.3

2.0 * 10-6 230 3.6

2.2 * 10-7 78 11

1.0 * 10-7 42 13

5.0 * 10-6 280 1.8

3.0 * 10-6 340 3.6

1.9 * 10-7 76 13

1.0 * 10-7 44 14

25

Protection of the StaffProtection of the Staff

accelerator operation:

• stray radiation fields

(shielding , interlocks)

maintenance time:

• residual radioactivity

(choice of material, shielding)

• radioactive air

(ventilation concept)

26

Protection of the StaffProtection of the Staff

personal doses < 6 mSv / a

(2000 h working time)

local doses < 15 mSv / a

(5000 h operation time) =

local doses < 1,5 mSv / a

27

Protection of the StaffProtection of the Staff

personal doses < 20 mSv / a

local dose rates < 3 mSv / hOnly

temporary access

ALARA

28

Residual RadioactivityResidual Radioactivity

Hot spotsHot spots

29

Radioactivity of the tunnel airRadioactivity of the tunnel air

30

ConclusionsConclusions

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