Planning and preparation approaches for non-nuclear waste disposal

Similar documents
Radiation protection considerations along a radioactive ion beam transport line

SOURCES of RADIOACTIVITY

Chapter 3: Neutron Activation and Isotope Analysis

SPES cyclotron-driven fast neutron irradiation facility aimed at nuclear data needs for next generation nuclear reactors: the FARETRA project at LNL

Il progetto SPES: produzione di fasci di ioni radioattivi ai Laboratori Nazionali di Legnaro.

Review of ISOL-type Radioactive Beam Facilities

CALCULATION OF ISOTOPIC COMPOSITION DURING CONTINUOUS IRRADIATION AND SUBSEQUENT DECAY IN BIOLOGICAL SHIELD OF THE TRIGA MARK ΙΙ REACTOR

Radiation safety of the Danish Center for Proton Therapy (DCPT) Lars Hjorth Præstegaard Dept. of Medical Physics, Aarhus University Hospital

Activation of Air and Concrete in Medical Isotope Production Cyclotron Facilities

Evaluation of Radiation Characteristics of Spent RBMK-1500 Nuclear Fuel Storage Casks during Very Long Term Storage

Activation Analysis. Characteristic decay mechanisms, α, β, γ Activity A reveals the abundance N:

ACTIVATION ANALYSIS OF DECOMISSIONING OPERATIONS FOR RESEARCH REACTORS

Chem 1A Chapter 5 and 21 Practice Test Grosser ( )

Interaction of the radiation with a molecule knocks an electron from the molecule. a. Molecule ¾ ¾ ¾ ion + e -

1. RADIOACTIVITY AND RADIATION PROTECTION

SPES Conceptual Design Report

INVESTIGATION OF THE INTERMEDIATE NEUTRON CAPTURE ON UNSTABLE NUCLIDES BY MEANS OF THE ACTIVATION METHOD. Abstract

Nuclear Radiation. Natural Radioactivity. A person working with radioisotopes wears protective clothing and gloves and stands behind a shield.

D) g. 2. In which pair do the particles have approximately the same mass?

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of?

General, Organic, and Biological Chemistry, 3e (Frost) Chapter 2 Atoms and Radioactivity. 2.1 Multiple-Choice

Regents review Nuclear Chemistry

COMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS

7 th FLUKA Course NEA Paris, Sept.29-Oct.3, 2008

Chapter 21 Nuclear Chemistry

Sample Examination Questions

Hospital Cyclotrons: Radiation Safety Aspects. Matthew Griffiths

Depth Distribution of H-3, C-14 and Co-60 in Decommissioning of the Biological Shielding Concrete of KRR-2

Cross-section Measurements of Relativistic Deuteron Reactions on Copper by Activation Method

European Organisation for Nuclear Research European Laboratory for Particle Physics

Chemistry 52 Chapter 11 ATOMIC STRUCTURE. The general designation for an atom is shown below:

Alpha Decay. Decay alpha particles are monoenergetic. Nuclides with A>150 are unstable against alpha decay. E α = Q (1-4/A)

NJCTL.org 2015 AP Physics 2 Nuclear Physics

Differentiating Chemical Reactions from Nuclear Reactions

UNIT 13: NUCLEAR CHEMISTRY

There are no stable isotopes of elements above atomic number 83.

Neutron induced reaction and neutron sources

Predicting Long-Lived, Neutron-Induced Activation of Concrete in a Cyclotron Vault

Isotopes Atoms of an element (same # p+) that differ in their number of neutrons

Chapter 30 Questions 8. Quoting from section 30-3, K radioactivity was found in every case to be unaffected

Units and Definition

Key Question: What role did the study of radioactivity play in learning more about atoms?

Nuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic

Unit 2 Exam - Atomic Structure and Nuclear

The LENOS project at Laboratori Nazionali di Legnaro of INFN: a thermal to 70 MeV neutron beam facility

At the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation.

Homework 06. Nuclear

MockTime.com. Ans: (b) Q6. Curie is a unit of [1989] (a) energy of gamma-rays (b) half-life (c) radioactivity (d) intensity of gamma-rays Ans: (c)

Provisional scenario of radioactive waste management for DEMO

Number of protons. 2. What is the nuclear symbol for a radioactive isotope of copper with a mass number of 60? A) Cu

The residual radioactivity of a water-copper beam dump for the TESLA Test Facility

Radioactivity Review (Chapter 7)

Sources of Radiation

Induced Radioactivity. Beginners FLUKA Course

Write down the nuclear equation that represents the decay of neptunium 239 into plutonium 239.

MEASUREMENT OF SPENT FUEL ASSEMBLIES IN SPRR-300

Nuclear and Radiation Physics

Chapter 21. Chemistry, The Central Science, 10th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten

Activity # 2. Name. Date due. Assignment on Atomic Structure

General, Organic, and Biochemistry, 2e (Frost) Chapter 2 Atoms and Radioactivity. 2.1 Multiple-Choice

Gamma and X-Ray Standards

PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY

Introduction to Ionizing Radiation

Current issues of radiation safety regulation for accelerator facilities in Japan

the properties of that element

CHAPTER 7 TEST REVIEW

Calculation of the Dose Equivalent Rate from Induced Radioactivity Around the CNGS Target and Magnetic Horn

Neutron Dose near Spent Nuclear Fuel and HAW after the 2007 ICRP Recommendations

Particle Size of Radioactive Aerosols Generated During Machine Operation in High-energy Proton Accelerators

Laser Spectroscopy on Bunched Radioactive Ion Beams

neutrons in the few kev to several MeV Neutrons are generated over a wide range of energies by a variety of different processes.

Application of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers

6 Neutrons and Neutron Interactions

Phys102 Lecture 29, 30, 31 Nuclear Physics and Radioactivity

Internal Report DESY D3-86 January Production of radioactive nuclides in soil and groundwater near the beam dump of a Linear Collider. K.

Lecture 31 Chapter 22, Sections 3-5 Nuclear Reactions. Nuclear Decay Kinetics Fission Reactions Fusion Reactions

Chapter 18. Nuclear Chemistry

The heavy-ion magnetic spectrometer PRISMA

da u g ht er + radiation

SPES secondary beam planning

Activation Products in Proton Therapy

Nuclear Chemistry. In this chapter we will look at two types of nuclear reactions.

1. Which is the most commonly used molten metal for cooling of nuclear reactors? A. Zinc B. Sodium C. Calcium D. Mercury


Pete Burgess, Nuvia Limited. Clearance and exemption

When a body is accelerating, the resultant force acting on it is equal to its

QUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter

Lecture Presentation. Chapter 21. Nuclear Chemistry. James F. Kirby Quinnipiac University Hamden, CT Pearson Education, Inc.

[2] State in what form the energy is released in such a reaction.... [1]

Atoms and Nuclear Chemistry. Atoms Isotopes Calculating Average Atomic Mass Radioactivity

Activity 12 Isotopes and Radioactivity

Neutron Shielding Materials

In the Beginning. After about three minutes the temperature had cooled even further, so that neutrons were able to combine with 1 H to form 2 H;

SLAC Metal Clearance Program and Progress

Introduction to neutron sources

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams

EXPERIMENTAL STUDY OF NEUTRON FIELDS PRODUCED IN PROTON REACTIONS WITH HEAVY TARGETS. Nuclear Physics Institute AS CR, Rez Czech Republic

3 Radioactivity - Spontaneous Nuclear Processes

A. Element 1. The number of protons and neutrons of an atom.

Chapter 10. Answers to examination-style questions. Answers Marks Examiner s tips. 1 (a) (i) 238. (ii) β particle(s) 1 Electron antineutrinos 1

Transcription:

Planning and preparation approaches for non-nuclear waste disposal Lucia Sarchiapone Laboratori Nazionali di Legnaro (Pd) Istituto Nazionale di Fisica Nucleare INFN Lucia.Sarchiapone@lnl.infn.it +39 049 8068 394

Outline Laboratori Nazionali di Legnaro The SPES Project Expected levels of radioactivity, studies: The irradiation target The shielding structure Approach for the disposal NEA Workshop on the Management of Non-nuclear Radioactive Waste 2

NEA Workshop on the Management of Non-nuclear Radioactive Waste New building area hosting the cyclotron and the irradiation bunkers Existing acceleration line Linear accelerator ALPI 3

The SPES Project (Selective Production of Exotic Species) Radioactive Cyclotron ALPI beams: 90 Rb, 135 I, 137 Te, 138 Xe, 94 Kr, 132 Sn, 134 Sn PIAVE TANDEM RIB: Sn-132 +n, I-135 +n, 9 MeV/amu RIB: Sn-132 +n, I-135 +n, up to 40 kv RIB: Sn-132 +1, I-135 +1, up to 40 kv according to mass Protons, 40 MeV 200 ma NEA Workshop on the Management of Non-nuclear Radioactive Waste 4

The Cyclotron name: p70 made by: Best Cyclotron energy: 40-70 MeV maximum current: 750 ua particles: H- special remarks: dual port NEA Workshop on the Management of Non-nuclear Radioactive Waste 5

The fissionable target Graphite holder 7 UC 2 disks 1 mm thick Graphite dump Developed by the SPES target group, www.lnl.infn.it/~spes_target/ NEA Workshop on the Management of Non-nuclear Radioactive Waste 6

Target ISOL technique beam effusion at work Ionization of the radioactive beam The type of source is related to the final beam NEA Workshop on the Management of Non-nuclear Radioactive Waste A. Andrighetto 7

Fluka geometry The target: irradiation cycle and inventory The SPES target is made of 7 UCx disks, 4 cm diameter, 1 mm thickness (about 30 g uranium-238 content) Graphite box Proton beam window UC x disk dumper The irradiation cycle lasts 14 days, a total of 10 21 protons on target and a total of 10 19 fissions are induced on the target NEA Workshop on the Management of Non-nuclear Radioactive Waste 8

Atomic abundances (atoms per 200 ua) atomic abundance (atoms per 200uA) Atomic number Z Z Atoms atoms per per proton proton Production in production target at in target 40 at MeV 40 proton energy 100 The target: irradiation cycle and inventory 90 10-1 10-2 80 10-3 Direct fission from 40 MeV protons on UC 2 70 60 50 40 10-4 10-5 10-6 10-7 10 12 30 20 10-8 10-9 10 10-10 10 11 0 0 20 40 60 80 100 120 140 N Number of neutrons N 10-11 FLUKA simulation 10 10 10 13 fissions/sec 10 9 60 80 100 120 140 160 180 mass number (A) Mass number A Total target activity after 2 weeks irradiation 3.7 10 13 Bq NEA Workshop on the Management of Non-nuclear Radioactive Waste 9

The target: irradiation cycle and inventory 14 days 10 21 protons on target 10 19 fissions/cycle About 1 kci totally produced in 1 cycle 10% 1% 2% T 1/2 < 1 hour 1 hour < T 1/2 < 1 day 1 day < T 1/2 < 1 month 1 month < T 1/2 < 1 year 1 year < T 1/2 < 10 years T 1/2 > 10 years 17% 70% NEA Workshop on the Management of Non-nuclear Radioactive Waste 10

The target: induced radioactivity Bq NEA Workshop on the Management of Non-nuclear Radioactive Waste 11

The temporary storage design Small area to store the irradiated targets before their final destination as waste NEA Workshop on the Management of Non-nuclear Radioactive Waste 12

Simulation set up Lead and steel box, as designed and realized by the target group at LNL NEA Workshop on the Management of Non-nuclear Radioactive Waste 13

Y (cm) RP consideration on temporary storage 800 700 600 500 400 300 200 100 0 Gamma dose rate from exhausted targets Ceiling floor -100 2800 3200 3600 4000 4400 X (cm) < 50 msv/h Once filled the rack, targets will shield each other: dose rate below 50 usv/h A concrete wall 50 cm thick will reduce the dose rate by a factor 100 msv/h 10 7 10 6 10 5 10 4 10 3 10 2 10 1 10-1 10-2 NEA Workshop on the Management of Non-nuclear Radioactive Waste 14

Irradiation process the shielding UC 2 target (30 g) in the form of 7 thin disks. Energy: 40 MeV Current: 200 ma Irradiation period: 20 years Working load: 5000 hours/year target 2 m distant from the wall surface; shielding wall 360 cm wide; UC 2 cylindrical activation sample cut in the wall, radius 3 cm, zero degree parallel to the beam direction p 40MeV 200 ma NEA Workshop on the Management of Non-nuclear Radioactive Waste 15

Shielding Material Elemental composition of concrete (r=2.3 g/cm 3 ) used for the shielding of the target hall: Hydrogen underestimated (conservative assumption neutron slowing down effect); Eu and Co important because of their long half lives; Iron percentage does not include that due to the reinforcement rods. Element Atomic Fraction Weight Fraction Hydrogen 0.1047 0.55% Oxygen 0.584 48.91% Magnesium 0.0157 2.0% Aluminum 0.0317 4.48% Silicon 0.2115 31.1% Calcium 0.0479 10.05% Iron 0.01 2.92% Europium 3.7 10-8 0.294 ppm Cobalt 0.826 10-6 2.55 ppm Reinforcement is obtained with a stainless steel grid, with rods of radius 1 cm, spaced by 10 cm. NEA Workshop on the Management of Non-nuclear Radioactive Waste 16

cm -2 per proton Neutron fluence p 40MeV 200 ma UC 2 NEA Workshop on the Management of Non-nuclear Radioactive Waste 17

Neutron energy Reactions of neutrons with nuclei in the shielding: Thermal neutrons (E < 1 ev) High energy neutrons (E > 20 MeV) NEA Workshop on the Management of Non-nuclear Radioactive Waste 18

Neutron energy and radioactive species Some long lived radionuclides are produced by high energy neutrons ( 54 Mn, 22 Na) 54 Mn 54 Fe (n,p) 55 Mn (n,2n) 22 Na 23 Na (n,2n) NEA Workshop on the Management of Non-nuclear Radioactive Waste 19

Neutron energy and radioactive species Some radionuclides produced by thermal neutrons: the activity concentration as a function of the depth in concrete resembles that of thermal flux. 46 Sc 45 Sc (n,g) 59 Fe 58 Fe (n,g) 60 Co 59 Co (n,g) 152 Eu 151 Eu (n,g) NEA Workshop on the Management of Non-nuclear Radioactive Waste 20

Radioactive species in concrete Following the irradiation of the concrete structure by secondary neutrons, nuclei de-excite by the emission of energetic g-rays; Nuclide Half life 152 Eu 13.5 y 60 Co 5.27 y 59 Fe 44.5 d 56 Co 77.27 d g-ray energy (kev) 121.78 1408.01 1173.24 1332.5 1099.22 1291.56 846.7 1238.0 Table: Radionuclides with T 1/2 > 1 month. The more energetic g emitters have been included. 54 Mn 312.12 d 834.83 46 Sc 83.79 d 26 Al 7.4 10 5 y 889.25 1120.51 1808.0 1129.0 22 Na 2.602 y 1274.54 NEA Workshop on the Management of Non-nuclear Radioactive Waste 21

Radioactive species in concrete Long lived radionuclides in a sample 20 cm deep from the surface, at the end of the irradiation period (20 years). Nuclide Half life 152 Eu 13.5 y 60 Co 5.27 y Activity (Bq/g) 232.7 172.7 6% of the overall activity is due to nuclides with half life longer than 1 year. The nuclides specified in the table are found in the concrete sample. In the rods some of these nuclides can be found (species produced by irradiation of iron, 60 Co, 59 Fe, 55 Fe, 54 Mn) with higher concentrations. 59 Fe 44.5 d 137.8 55 Fe 2.73 y 1.2 10 4 54 Mn 312.12 d 1.5 10 3 45 Ca 162.61 d 1.0 10 4 26 Al 7.4 10 5 y 216.0 22 Na 2.602 y 223.0 3 H 12.33 y 1.4 10 3 NEA Workshop on the Management of Non-nuclear Radioactive Waste 22

Activation and cooling Activity concentration rapidly decays as the depth increases in the first 20-30 cm. Symbols represent the activity concentration in the rods, while lines represent the same quantity in concrete. As a representative value, 1Bq/g is obtained after 20 years of cooling time in the outer part 185 cm thick. NEA Workshop on the Management of Non-nuclear Radioactive Waste 23

Conclusions LNL host particles accelerators for research in nuclear physics New projects and high power involved push for consideration of waste production and planning for disposal Necessary to start the study before civil construction starts, in order to plan places and techniques for future disposal. NEA Workshop on the Management of Non-nuclear Radioactive Waste 24

Thank you for your attention L. Sarchiapone Laboratori Nazionali di Legnaro (Pd) Istituto Nazionale di Fisica Nucleare INFN Lucia.Sarchiapone@lnl.infn.it NEA Workshop on the Management of Non-nuclear Radioactive Waste 25 +39 049 8068 394