new materials for radiation protection buildings monte carlo-simulations and measurement for
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New materials for radiation protection buildings Monte Carlo-simulations and measurement for X-rays, Protons, and Carbon ions. a cooperation between university and industry. Reinhold G. Müller, Nils Achterberg, Jürgen Karg Inst. Med. Physik, Strahlenklinik Universität Erlangen. - PowerPoint PPT PresentationTRANSCRIPT
Strahlenklinik ErlangenSATIF 2010 CERN
New materials for radiation protection buildings
Monte Carlo-simulations and measurement for
X-rays, Protons, and Carbon ions
Reinhold G. Müller,Nils Achterberg,Jürgen KargInst. Med. Physik,StrahlenklinikUniversität Erlangen
Jan Forster,Renate ForsterIngenieurgesellschaftIngolstadt
a cooperation between university and industry
Otto Pravida,Pravida Bau GmbHPressath
Strahlenklinik ErlangenSATIF 2010 CERN
wall structure of Sandwich
30 - 40 30 - 4060 - >900 cm
variablevariablefilling materials and mixturesfilling materials and mixtures
double wall shellfilled with concrete
Strahlenklinik ErlangenSATIF 2010 CERN
concrete of appropriate thickness is widely used forshielding walls:
advantage: concrete is available everywhere and not too expensive;
dis- - concrete needs shuttering and reinforcement;advantage: - long dry out time; - cracking in spite of reinforcement; - for enhancing density aggregates like Baryt are necessary, which increase the costs, up to a factor of 10; - shielding structures of more than 6 m thickness (high energy physics) make cooling necessary because of the process heat during hardening; - dismantling of these structures is very expensive.
state of the art
Strahlenklinik ErlangenSATIF 2010 CERN
There is no need for such heavy constructions because of statics. Radiation protection can be reached more efficient and for significant reduced prices using adequate filling.That‘s why the Sandwich construction has been developed.
advantage: - precast technology, nearly dry;
- shielding by natural minerals like gypsum or limestone (low costs);
- ceiling construction in same manner;
- erection time less than 1/3 in relation to concrete;
- for density enhancement natural minerals like iron-ore,
Magnetit, Baryt, iron-slag, etc. can be aggregated (low costs);
- optimal combinations are possible for nearly all problems;
- the high content of crystal water qualifies gypsum for the
attenuation of primary and secondary neutrons;
- dismantling of the construction and reinstatement can easily
be done with simple techniques;
disadvantage: - none -
the technical innovation: Sandwich Construction
Strahlenklinik ErlangenSATIF 2010 CERN
6, 10 u. 15MV; KD + ONCOR05.-06.08. 2005
1,E-03
1,E-02
1,E-01
1,E+00
0 50 100 150 200 250
Area density [ g/cm² ]
Tra
ns
mis
sio
n
slag 6MV KD
slag 10 MV KD
slag 6MV ONCOR
slag 15 MV ONCOR
measurement and results
suitable for DIN 6847-2 (German regulations, Sept. 2008)
and NCRP 144, 153 (American regulations)
Strahlenklinik ErlangenSATIF 2010 CERN
Tenth value layer [ g/cm² ]
20
40
60
80
100
120
1 10 100
Maximum energy [MeV ]
Te
nth
va
lue
lay
er
[ g
/cm
² ]
Concrete DIN (~2,3)
Concrete + MD2 (~3,5-3,8)
EOS-MC + Measurement (~2,5)
Barytbeton (~3,5-3,8)
tenth value layers tvl
DIN 6847-2, NCRP
Strahlenklinik ErlangenSATIF 2010 CERN
materials under investigation
1. 3 kinds of normal concrete < 2.3 t/m³ (limestone concrete, mixed, silicate concrete)
2. magnetite concrete 3.5-3,8 t/m³
3. magnetite concrete with iron gravel 5.0 t/m³
4. natural gypsum 1.8 t/m³
5. limestone 1.9 t/m³
6. screen glass - - -
7. iron processing waste (Electric Arc Funrace Slag) 2.4 t/m³
8. magnetite pure (iron ore) 2.5 t/m³
Strahlenklinik ErlangenSATIF 2010 CERN
Datum: 2008 September
German Regulations: DIN 6847-2
Strahlenklinik ErlangenSATIF 2010 CERN
erection of a double wall shellsfor 8 vaults at once
closing of the bunkers&
filling the walls
Strahlenklinik ErlangenSATIF 2010 CERN
planning a huge vault
Strahlenklinik ErlangenSATIF 2010 CERN
erection of a huge vault
Strahlenklinik ErlangenSATIF 2010 CERN
filling optimised material mixtures
Strahlenklinik ErlangenSATIF 2010 CERN
closing the ceiling
Strahlenklinik ErlangenSATIF 2010 CERN
Datum: 2008 Januar
vaults for particle therapy
Strahlenklinik ErlangenSATIF 2010 CERN
walls made with concreteconcrete
MC-simulations for protons 220 MeV
neutron“volume dose”
E/V[ J/cm³ ]
GEANT4 7.1 S. Agostinelli et al. 2003, Nucl.Instrum.Methods A 506 250-303
Strahlenklinik ErlangenSATIF 2010 CERN
protons 220 MeV
neutron“volume dose”
E/V[ J/cm³ ]
walls in Sandwich TechnologySandwich Technology
Strahlenklinik ErlangenSATIF 2010 CERN
550 cm 600 cm 550 cm
carbon ions 430 MeV/u
walls with concreteconcrete
Strahlenklinik ErlangenSATIF 2010 CERN
550 cm 600 cm 550 cmwalls in Sandwich TechnologySandwich Technology
carbon ions 430 MeV/u
Strahlenklinik ErlangenSATIF 2010 CERN
deuterons 45 MeV
walls in Sandwich TechnologySandwich Technology
graphite target
Strahlenklinik ErlangenSATIF 2010 CERN
n(E) of carbon ions 430 MeV/uneutron spectra
neutron spectra
direction 0°
concreteconcrete
Strahlenklinik ErlangenSATIF 2010 CERN
Sandwich TechnologySandwich Technology
neutron spectra
direction 0°
n(E) of carbon ions 430 MeV/uneutron spectra
Strahlenklinik ErlangenSATIF 2010 CERN
convolution with RBE for calculation of H*(10) for neutrons
Strahlenklinik ErlangenSATIF 2010 CERN
effective dose H*(10) behind the wall of Sandwich TechnologySandwich Technology
protons 220 MeV
effective Dose H*(10)
direction 0°;same for mixture or concrete
TVL: 109 cm resp. 251 g/cm²
Strahlenklinik ErlangenSATIF 2010 CERN
attenuation measurement at GSI
igloo
beam line
targets
0°
45°
90°
windows
filling material
3 different at once
6 different in total
3 wendi2 detectors
neutron dose H*(10)
p+
carbon ions
Strahlenklinik ErlangenSATIF 2010 CERN
igloo installed at GSI
0°45°
Strahlenklinik ErlangenSATIF 2010 CERN
Sandwich TechnologySandwich Technology
protons 220 MeV
effective dose H*(10) per 109 protons behind (inside) the wall depending on energy and angle
measurement
MC-simulation angle °
Strahlenklinik ErlangenSATIF 2010 CERN
normalized to the entrance value, depending on energy and angle
effective neutron dose H*(10) for protons behind (inside) the wall
MC-simulation
angle °
Strahlenklinik ErlangenSATIF 2010 CERN
MC-simulation
effective neutron dose H*(10) for protons behind (inside) the wall
normalized to the entrance value,
E = 220 MeV; angle = 0°
Strahlenklinik ErlangenSATIF 2010 CERN
430 MeV/u Carbon 0°
y = 273035e-0,005x
R2 = 0,9957
y = 471441e-0,0074x
R2 = 0,9885
y = 372908e-0,0063x
R2 = 0,9941
y = 492832e-0,0076x
R2 = 0,9902
y = 459420e-0,0073x
R2 = 0,9908
y = 496779e-0,0076x
R2 = 0,9934
1,E+02
1,E+03
1,E+04
1,E+05
1,E+06
0 200 400 600 800 1000
Areal Density / g/cm²
H*(
10
) / n
Sv
/10
^6
Ion
s
Concrete 2
EAS
Gypsum
Magnetite
Limestone
Asphalt
Borax
300 MeV/u Carbon 0°
y = 57886e-0,005x
R2 = 0,9998
y = 95801e-0,0073x
R2 = 0,9958
y = 78056e-0,0063x
R2 = 0,9996
y = 99219e-0,0074x
R2 = 0,9976
y = 94803e-0,0073x
R2 = 0,9969
y = 98035e-0,0073x
R2 = 0,9932
1,E+02
1,E+03
1,E+04
1,E+05
1,E+06
0 200 400 600 800 1000
Areal Density / g/cm²
H*(
10) /
nS
v/10
^6 Io
ns
Concrete 2
EAS
Gypsum
Magnetite
Limestone
Asphalt
Borax
200 MeV/u Carbon 0°
y = 11255e-0,0054x
R2 = 0,9997
y = 20155e-0,0082x
R2 = 0,9947
y = 15599e-0,0068x
R2 = 0,9996
y = 21045e-0,0083x
R2 = 0,9971
y = 20034e-0,0082x
R2 = 0,9976
y = 23174e-0,0087x
R2 = 0,9901
1,E+01
1,E+02
1,E+03
1,E+04
1,E+05
0 200 400 600 800 1000
H*(
10
) / n
Sv
/10
^6
Ion
s
Concrete 2
EAS
Gypsum
Magnetite
Limestone
Asphalt
Borax
Areal Density / g/cm³
150 MeV/u Carbon 0°
y = 2676,9e-0,0062x
R2 = 0,9912
y = 3651,5e-0,0076x
R2 = 0,999
y = 5244,5e-0,0091x
R2 = 0,9987
y = 5239,3e-0,0094x
R2 = 0,9992
y = 5725,6e-0,0095x
R2 = 0,9984
y = 4320,6e-0,0084x
R2 = 0,9974
1,E+00
1,E+01
1,E+02
1,E+03
1,E+04
0 200 400 600 800 1000
Areal Density / g/cm³
H*(
10
) / n
Sv/
10
^6 Io
ns
Concrete 2
EAS
Gypsum
Magnetite
Limestone
Asphalt
Borax
effective neutron dose H*(10) for carbon ionsbehind the wall; measurement
5 cm Borax
Strahlenklinik ErlangenSATIF 2010 CERN
0° TVL for Carbon Ions
200
300
400
500
600
100 150 200 250 300 350 400 450 500
Energy Carbon Ion / MeV/u
TV
L /
g/c
m²
0° Concrete
0° EAS
0° Gypsum
0° Magnetite
0° Limestone
0° Asphalt
tenth value layers TVL for neutron dose H*(10) for carbon ions behind the wall
Strahlenklinik ErlangenSATIF 2010 CERN
the Sandwich Constructionis suitable for all radiation sources,
and satisfies all requirements with a variety of advantages
as for example:
1. cost reduction;
2. reduced erection time;
3. flexible adjustment to the aspired wall thickness
because of the free option of filling material;
4. feasibility of building alterations;
5. simple and cheap dismantling and reinstatement;
conclusion
Strahlenklinik ErlangenSATIF 2010 CERN
the
end
thank you for your attention