DETERMINATION OF THE HYDROGEN CONTENT OF OIL SAMPLES FROM NIGERIA USING AN Am-Be NEUTRON SOURCE.

Similar documents
Physics Dept. PHY-503-SEMESTER 112 PROJECT. Measurement of Carbon Concentration in Bulk Hydrocarbon Samples

A Monte Carlo Simulation for Estimating of the Flux in a Novel Neutron Activation System using 252 Cf Source

Neutron Imaging System For level Interface Measurement

Introduction. 1. Neutron reflection cross section

Determination of the boron content in polyethylene samples using the reactor Orphée

Measurement of Average Thermal Neutron Flux for PGNAA Setup

MULTI-ELEMENTAL ANALYSIS OF SOME NIGERIAN MINERAL ROCKS FOR A COMPARATIVE ASSAY OF GAMMA SHIELDING WITH CONCRETE USING WINXCOM

DETERMINATION OF NEUTRON-INDUCED ACTIVATION CROSS SECTIONS USING NIRR-1

Distinguishing fissions of 232 Th, 237 Np and 238 U with beta-delayed gamma rays

Determination of Absorbed and Effective Dose from Natural Background Radiation around a Nuclear Research Facility

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

Pulsed Neutron Interrogation Test Assembly - PUNITA

Collimated LaBr 3 detector response function in radioactivity analysis of nuclear waste drums

RARE EARTH ELEMENT DISTRIBUTION PATTERNS IN THE SOILS AROUND THE NIGERIAN RESEARCH REACTOR-1, (NIRR-1) IN ZARIA, NIGERIA

Section 3: Nuclear Radiation Today

PARAMETERISATION OF FISSION NEUTRON SPECTRA (TRIGA REACTOR) FOR NEUTRON ACTIVATION WITHOUT THE USED OF STANDARD

WM2014 Conference, March 2 6, 2014, Phoenix, Arizona, USA

MC simulation of a PGNAA system for on-line cement analysis

DOE SBIR & STTR FY 2019 Phase 1, Release 1 Topics

International Journal of Scientific & Engineering Research, Volume 5, Issue 3, March-2014 ISSN

Digital simulation of neutron and gamma measurement devices

MEASUREMENT OF SPENT FUEL ASSEMBLIES IN SPRR-300

Development of Continuous Inflow Tritium in Water Measurement Technology by using Electrolysis and Plastic Scintillator

"Neutron Flux Distribution"

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

Unit 3(a) Introduction to Organic Chemistry

Simulated Results for Neutron Radiations Shielding Using Monte Carlo C.E. Okon *1, I. O. Akpan 2 *1 School of Physics & Astronomy,

Radioactivity III: Measurement of Half Life.

Activities of the neutron standardization. at the Korea Research Institute of Standards and Science (KRISS)

Measurement of linear and mass attenuation coefficient of alcohol soluble compound for gamma rays at energy MeV

HANAA* Humans Applying Neutron Activation Analysis Hassan Amany Noura Ahmed Ali

Evaluation of Nondestructive Assay Characterization Methods for Pipe- Over-Pack Containers

WM2014 Conference, March 2 6, 2014, Phoenix, Arizona, USA

Measurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory

VERIFICATION OF MONTE CARLO CALCULATIONS OF THE NEUTRON FLUX IN THE CAROUSEL CHANNELS OF THE TRIGA MARK II REACTOR, LJUBLJANA

ɣ-radiochromatography

Validation of the MCNP computational model for neutron flux distribution with the neutron activation analysis measurement

CALIBRATION OF SCINTILLATION DETECTORS USING A DT GENERATOR Jarrod D. Edwards, Sara A. Pozzi, and John T. Mihalczo

Inaccuracy Determination in Mathematical Model of Labsocs Efficiency Calibration Program

12/18/2016. Radioanalysis Laboratory Capabilities and Issues. Eleventh Annual Radiation Measurement Cross Calibration Workshop RMCC XI

Neutron activation analysis. Contents. Introduction

THE ANNUAL EFFECTIVE DOSE FROM NATURAL RADIONUCLIDES SOIL SURFACES OF UZHGOROD AREA

FISSILE MATERIALS DETECTION VIA NEUTRON DIFFERENTIAL DIE-AWAY TECHNIQUE

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS

Recent improvements in on-site detection and identification of radioactive and nuclear material

Chem 481 Lecture Material 4/22/09

Journal of Chemical and Pharmaceutical Research, 2012, 4(1): Research Article

SECTION 8 Part I Typical Questions

Characteristics of Filtered Neutron Beam Energy Spectra at Dalat Reactor

5 Atomic Physics. 1 of the isotope remains. 1 minute, 4. Atomic Physics. 1. Radioactivity 2. The nuclear atom

International Journal of Scientific & Engineering Research Volume 9, Issue 1, January ISSN

On-Conveyor Belt Determination of Ash in Coal

Effect of Co-60 Single Escape Peak on Detection of Cs-137 in Analysis of Radionuclide from Research Reactor. Abstract

SPS Chapter Research Award Interim Report

CHAPTER 4 NUCLEONIC GAUGES. B.D. Sowerby

Gamma background measurements in the Boulby Underground Laboratory

European Project Metrology for Radioactive Waste Management

Alternative Approach for Efficiency Data Generation in Neutron Activation Analysis

DEVELOPMENT OF NEUTRON INTERROGATION TECHNIQUES TO DETECT DANGEROUS SUBSTANCES

1. INTRODUCTION 2. EAEA EXISTING CAPABILITIES AND FACILITIES

Applications of MCBEND

arxiv:nucl-ex/ v2 21 Jul 2005

Introduction to Ionizing Radiation

He-3 Neutron Detectors

Measurements of liquid xenon s response to low-energy particle interactions

Isotopes: atoms with the same Z but different A s (number of neutrons varies)

POSITION SENSITIVE DETECTION OF CONCEALED SUBSTANCES EMPLOYING PULSED SLOW NEUTRONS

ISOCS / LabSOCS. Calibration software for Gamma Spectroscopy

Library of uranium and plutonium reference spectra Introduction

Quality Assurance. Purity control. Polycrystalline Ingots

An Optimized Gamma-ray Densitometry Tool for Oil Products Determination

Non-Destructive Assay Applications Using Temperature-Stabilized Large Volume CeBr Detectors 14277

Nuclear Science Merit Badge Workbook

Simple Experimental Design for Calculation of Neutron Removal Cross Sections K. Groves 1 1) McMaster University, 1280 Main St. W, Hamilton, Canada.

THE COMPTON EFFECT Last Revised: January 5, 2007

Nuclear Fission. Q for 238 U + n 239 U is 4.??? MeV. E A for 239 U 6.6 MeV MeV neutrons are needed.

Radioactivity of the Treated Topaz

Name Date Class NUCLEAR CHEMISTRY

Higher -o-o-o- Past Paper questions o-o-o- 3.6 Radiation

POTASSIUM GEONEUTRINOS AND THEIR DETECTION

Characterization and Monte Carlo simulations for a CLYC detector

Name Date Class NUCLEAR RADIATION. alpha particle beta particle gamma ray

1 General information and technical data of TRIGA RC-1 reactor

IMAGING OF HETEROGENEOUS MATERIALS BY. P. Staples, T. H. Prettyman, and J. Lestone

Utilization of Egyptian Research Reactor and modes of collaboration

by V. Chisté and M. M. Bé


Procedure for Radio Dating of Water Using Nuclear Hydrological Isotopes Techniques

Overview of X-Ray Fluorescence Analysis

SYRACUSE UNIVERSITY RADIATION PROTECTION PROGRAM APPLICATION FOR USE OF RADIOACTIVE MATERIALS

A Brief Overview of Radiation and Analytical Water Testing for Radiological Contaminants.

COMPARATIVE STUDY BETWEEN EXTERNAL STANDARD METHOD AND INTERNAL STANDARD METHOD FOR LOW-LEVEL TRITIUM MEASUREMENTS

A Radiation Monitoring System With Capability of Gamma Imaging and Estimation of Exposure Dose Rate

The Best Gamma-Ray Detector

Ch05. Radiation. Energy and matter that comes from the nucleus of an atom. version 1.6

M.Cagnazzo Atominstitut, Vienna University of Technology Stadionallee 2, 1020 Wien, Austria

Figure 1: Two pressure shocks causing the sample temperature increase (Termocouple Tc1, figure 1b of reference [2]). 2 Heat production Apart from the

Measurements of Neutron Capture Cross Sections for 237, 238 Np

I-4. SANS BATAN: Improvement the Neutron Intensity by Focusing Optics

WM2013 Conference, February 24 28, 2013, Phoenix, Arizona, USA

Transcription:

XA9949522 DETERMINATION OF THE HYDROGEN CONTENT OF OIL SAMPLES FROM NIGERIA USING AN Am-Be NEUTRON SOURCE. S.A. JONAH 1 *, I.I. ZAKARI 2 and SB. ELEGBA 1 1 Centre for Energy Research and Training, Ahmadu Bello University, P.MB. 1014, Zaria, Nigeria. E-mail: jonah@abu.edu.ng, fax: 234 62 242227 2 Ahmadu Bello University, Zaria, Nigeria. * Chief Scientific Investigator ABSTRACT A 5 Ci Am-Be neutron source-based facility, which utilises the principles of thermal neutron reflection technique in combination with foil activation method, has been used to determine the total hydrogen content of commercial oil samples from Nigeria. With an established detection limit of 0.25 H w% for oil matrix of volume 600-ml, the total hydrogen contents of the samples were found to be in the range of 11.11-14.22 H w%. The facility is economical and suitable for the determination of moisture in solid samples. A brief description of the on-going projects and future plans concerning the CRP are enumerated. INTRODUCTION A knowledge of total hydrogen content of bulk materials is necessary in several areas of science and technology. In Nigeria, there is a growing interest in the mining industries where knowledge of the hydrogen/moisture contents of minerals is needed for plant quality control. Presently the industrial method of assaying hydrogen in different materials is destructive and entails long hours of analysis. Since in most cases, hydrogen needs to be measured in bulk media, the use of a nuclear analytical technique based on moderation of fast neutrons has been recommended [1]. The thermal neutron reflection technique which was developed by Buczko et al., [2] and used by a number of investigators [3], [4], [5], [6] and [7] was adapted for this work. A set-up based on a 5 Ci Am-Be neutron source which utilises activation foil as the neutron probe was developed for the determination of total hydrogen content in commercial oil samples from Nigeria. EXPERIMENTAL The experimental set-up shown in Figure 1 consists of a 5 Ci Am-Be neutron source embedded in a cylindrical paraffin block of diameter 30 cm and of height 30 cm. The extended paraffin block serves as a moderator and provides personnel shielding against radiation hazards. In order to increase the signal-to-background response, a 1-mm thick 1 Part of this work is to be published in Appl. Rad. & Isotopes NEXT PAGE(S) left BLANK

Sample Cd Sheet Am-Be Neutron Source -Paraffin FIG. 1 The experimental setup used for the determination of H content of the oil samples

arrangement the thermal neutron probe and the 5x5 cm cadmium sheet already fastened to the bottom of the container are placed directly on the source in a reproducible geometry. Relevant nuclear data for the high-purity indium foil of dimensions 15x10x1-mm, are given in Table 1. TABLE 1. Nuclear data of the thermal neutron flux detector. Reaction H5 In(n,y) 116ra In Halflife (min) 54.12 Cross section (b) 16.20 Gamma Energy (kev) 416.90 1097.30 1293.50 Gamma Intensity (%) 29.20 56.20 84.40 For a given mass of indium foil, the relative excess specific activity induced in the detector foil in the presence of a sample is related to the neutron reflection parameter (ri) as shown below: r\ = (A - Ao)/p. Ao (1) Where, p is the physical density of the sample, while A and Ao are the specific activities of thermal neutrons induced in the detector foil with and without the sample respectively. The sample is exposed to fast neutrons from the Am-Be source for one hour and the resulting intensity of thermal neutrons from the samples is monitored by an indium detector foil via the 115 In(n,y) I16m In reaction. Radioactivity measurements of the detector foils are carried out for 30 minutes by a gamma-ray spectrometric system after a cooling time of 20 minutes. The radioactivity measuring system consists of a 7.6x7.6 cm Nal(Tl) crystal scintillator detector coupled to a computer-based multi-channel analyser. Hydrocarbons in liquid form containing well-known hydrogen and carbon contents were used as standards to determine the calibration line shown in Figure 2. The measured (r\) values for the standards are presented in Table 2.

TABLE 2. Data of standard samples used to construct the calibration line. Standard P H (w%) (g/cm 3 ) CeH6 0.879 3.74 ±0.02 7.692 BENZENE C 7 H 8 0.866 4.11±0.02 8.696 TOLUENE (CH 3 )2CO 0.792 4.33±0.02 10.344 ACETONE H 2 O 1.000 4.60±0.02 11.110 WATER C 2 H 5 OH 0.790 4.9910.03 13.043 ETHANOL C4H10O 0.789 5.11+0.03 13.514 BUTYL- ALCOHOL C7H16 0.684 5.7010.03 16.000 n-heptane

RESULTS AND DISCUSSION The solid line in Figure 2 for the determination of total hydrogen content was derived by fitting equation 2 below. x\ -n 0 + m. H (w%) (2) Where, rj o = 2.030±0.092 represents the effect of the matrix and m= 28±0.012 is the slope of the calibration line for hydrogen determination. The total hydrogen content of the samples displayed in Table 3 were deduced using equation 2. These are the average values of the data obtained using the peak analysis reports of the 416.9, 1097.3 and 1293.5 kev gamma lines respectively. Results show that the hydrogen content increases as one moves from fuel oil to lubricants and also as one moves from spent lubricants to fresh lubricant. The hydrogen content of spent lubricants appears to decrease with usage as can be seen in the results indicating the possibility of using this set-up as a quality control facility. Further measurements currently in progress are designed to standardise the set-up for industrial applications most especially for the determination of moisture content in solid minerals and agricultural products.

5 10 15 Hydrogen content (wjk) FIG. 2 Calibration line for the determination of total H content in oil samples

TABLE 3. Deduced hydrogen w% in the samples. Sample Petrol Kerosine Lubricant 1 Lubricant 2 Lubricant 3 Lubricant 4 Lubricant 5 Spent lubricant 2 (5000 km) Spent lubricant 2 (8000 km) P (g/cm 3 ) 0.744 0.794 0.835 0.867 0.842 0.855 0.864 0.897 0.898 H (w%) 12.30+0.15 12.26+0.15 14.22±0.17 13.54+0.16 13.38+0.16 12.78±0.15 11.11+0.13 12.62±0.15 11.48+0.14

Ill ON-GOING PROJECTS AND FUTURE PLANS 1. Modification of the set-up shown in FIG. 1 by replacing the indium foil with a Bf3 counter so as to increase the signal-to-background ratio and decrease the time for analysis. 2. Experimental studies in respect of a prompt-gamma neutron activation analysis (PGNAA) has started with the determination of the fast and thermal neutron flux density distributions inside a 30-cm square panel holder containing powdered coal samples. 3. Acquisition of the MNCP code to improve the PGNAA experimental set-up 4. Testing of the PGNAA facility using coal samples from Nigeria and Niger Republic. 5. Evaluation of the PGNAA facility using results obtained by the XRF technique 6. Development of an in-situ equipment for plant processing and control. REFERENCES [1] S. Semel and S. Helf, Int. J. Appld. Radiat. & Isot., 20,229, (1969) [2] M. Buczko, Z. Dezso and J. Csikai, J. Radioanal. Chem., 25, 179, (1975) [3] S. M. Al-Jobori, S. Szegedi and Cs. M. Buczko, Radiochem. Radioanal. Letts., 33, 133, (1978) [4] S. Szegedi and Z. Dezso Radiochem, Radioanal. Lett. 52, 343, (1982) [5] J. Csikai, Handbook on Fast Neutron Generators, CRC Press Inc., Boca Raton, Florida, (1987) [6] M. Yousif Ali, A.M. El-Megrab, S. A. Jonah, Daw May Su, M. Varadi and J. Csikai, Nuclear Geophysics, 9, 203, (1995) [7] S. A. Jonah, A. M. El-Megrab, M. Varadi and J. Csikai, J. Radioanal. & Nucl. Chem., 218, 193 (1997)