The International Department of Nuclear Physics, New Materials and Technologies has modern equipment for conducting laboratory exercises.
№ | Name of equipment | Brand of equipment, devices, etc. manufacturer, year of manufacture | Special purpose | Image |
1 | Seebeck coefficient and electrical resistance measuring system | Model ZEM-3 (M8) (RT up to 800 degree С) Apparatus: 220V and 100V, PC: 100V, GF-1С: 100V, Ulvac (Japan), 2015 | To conduct the Seebeck coefficient and electrical resistance of chalcogenide nanomaterials | |
2 | Fuel processor of electrochemical hydrogen processing device |
ВК-4-21.6-02; RP1DPF-10-F4N-H2; PMA-0,035 ГУЗ; PMA-0,25 ГУЗ. РХТУ (Russia), 2014 |
For the processing of storage, preparation and supply of fuel (hydrogen), as well as the supply of atmospheric air as an oxidizing agent | |
3 | Chemical Vacuum Station | РС 3012 NT Vario 743800 Vacuumbrand (Germany) 2013 | To solve the problems of evaporation in a large number of solvents | |
4 | An ultra-modern experimental setup for measuring the characteristics of SOFC and their materials at medium and high temperatures | 2017 | Installation for measuring the characteristics of fuel cells at medium and high temperatures | |
5 | Vacuum oven | CVF-1200 (Russia), 2016 | Gas-filled vacuum furnace for the synthesis and sintering of various materials in the field of hydrogen energy technologies | |
6 | LFA 467 HT measuring system | LFA 467 HT (Germany), 2017 | Equipment for measuring thermal conductivity, heat capacity and thermal conductivity of thin and highly conductive thermoelectric materials | |
7 | DSC 404 F1 measuring system | DSC calorimeter (Germany), 2017 | A differential scanning calorimeter is designated for studying thermal effects, phase transitions, studying enthalpy, determining heat capacity, conducting and studying differential thermal analysis of thermoelectric materials | |
8 | Chamber furnace LH 15/14 | Chamber stove (Germany), 2017 | Equipment for heat treatment, drying of solid samples, and for the synthesis of new energy functional materials | |
9 | Pull out drobe | Fume hood with ventilation system | For synthesis and laboratory chemical work | |
10 | Electronic scales AY 120 | Electronic scales AY 120 | For highly accurate weight measurements of samples | |
11 | Modern Test Bench Membrane Electrode Block - For Fuel Cells at Low Temperatures | Test bench for fuel cells at low temperatures | Installation for the study of materials of fuel cells of hydrogen energy | |
12 | Impedance meter | Solartron (England), 2017 | A device for characterizing fuel cells | |
13 | UV Spectrophotometer Jasco V 770 | Jasco Corp., Japan, 2015 | To obtain spectral lines in the UV region | |
14 | IR, Fourier spectrometer Jasco FTIR 4700 | Jasco Corp., Japan | For multicomponent gas analysis | |
15 | Experimental complex for measuring electrical parameters of solar cells PVIV Corp. made in USA | PVIV Corp, USA, 2014 | Used to measure the electrical parameters of solar cells | |
16 | Experimental complex based on MDR41 monochromator for measuring photoluminescence for liquid and solid samples | ОКB Spectrum, 2013 | To study the photoluminescence of liquid and solid samples | |
17 | An experimental complex based on a vacuum monochromator in vacuum ultraviolet spectroscopy in the energy range 2.0-12.0 eV at ultra low temperatures | Heraeus Noblelight GmbH, Germany, 2014 | To conduct experiments on obtaining spectra in the UV region in a vacuum | |
18 | Spectrofluorimeter SM2203 | СМ2203, ЗОА «SOLAR», 2011 | To determine the concentration of substances by fluorimetric methods in liquid and solid samples in the spectral region of 220-820 nm | |
19 | VUV radiation source | VUV200, Heraeus Noblelight GmbH, Germany, 2012 | For VUV analysis | |
20 | Monochromators | MDR41, 2012, MDR 204, 2009, MDR 23U, 1993 ОКB Spectrum | Far-ultraviolet spectral studies carried out in a vacuum | |
21 | Cryostat for low temperatures up to - 2000С | 1991 | Designed to maintain a given temperature of the liquid coolant circulating in the inner bath of the cryostat and in connected external consumers | |
22 | Thermoluminescent dosimetric system for individual control | SAPPHIRE 001, 2006 | To measure the dose of luminescence |
Search dosimeter-radiometer
MKS/SRP-08А
Purpose
The device is designed to measure the ambient dose equivalent of photon and neutron ionizing radiation, as well as the flux density of ionizing particles from alpha and beta radiation sources.
Technical characteristics
Detector |
gamma radiation: scintillation CsI (Na) or NaI (Tl) alpha, beta radiation: Geiger-Muller counter |
Range of measured values: | |
gamma and x-ray radiation ambient dose equivalent rate
flux density of alpha particles flux density of beta-particles |
0,1 ÷ 500 μSv/h 0,1 ÷ 700 cm-2s-1 0,1 ÷ 700 cm-2s-1
|
Energy range: | |
gamma and X-ray radiation alpha radiation beta radiation |
0,05 ÷ 3,0 MeV 3 ÷ 10 MeV 0,1 ÷ 3,5 MeV |
Limits of permissible basic relative measurement error: | |
gamma and x-ray radiation ambient dose equivalent rate flux density of alpha and beta particles |
± 15% ± 20% |
Sensitivity to gamma and x-ray radiation along the 662 keV line | 300 (pulse/s)/(μSv/h) |
Energy dependence of the sensitivity relative to the effective energy of 662 Kev, not more than | 25% |
Information output |
digital display of the results of measurement of the ambient dose equivalent of gamma and x-ray radiation (μSv/h) or pulse counting rate (pulse/s) digital display of the results of measurement of the alpha or beta particle flux density intensimeter - measuring path loading scale (analogous to arrow indication) audible alarm: - to search for sources via headphones - in monitor mode - siren |
Operating temperature | -20 ÷ +40°C |
Structural performance |
- the remote control in a plastic case and the detection unit are mounted on the wall - easily removable and carried by hand to locate contamination and sources
|
Power supply | 4 AA batteries |
Continuous operation time without charging, not less than | 15 hours |
Completeness
- electronic control unit for dosimeter-radiometer
- the detection unit BDPS-02A
- charger ZU-01
- control source 137Cs
- detector mount
- connecting cable
- telescopic rod
- mount to the electronic unit to the rod
Spectrometric installation
SKS-99 "Sputnik"
(with the BDFI-01 detection unit)
Purpose
SKS-99 is designed for measuring the activity and specific activity of beta-emitting radionuclides. SKS-99 can be used for solving radiation control problems during certification of food products.
Technical characteristics
The energy ranges of the detected radiations for | |
alpha radiation beta radiation neutron radiation: thermal neutrons, not less than intermediate and fast neutrons |
5х102 ÷ 9x103 keV 1,5х102 ÷ 4x103 keV
0,4 keV 1 ÷ 1,4x104 keV |
Ranges of measured activity for | |
integral specific activity of alpha-emitting radionuclides in "thick" samples integral activity of alpha-emitting radionuclides in "thin" samples activity surface (137Cs) |
1,5х102 ÷ 5x105 Bq/kg
10-2 ÷ 104 Bq 103 ÷ 106 Bq/m2 |
Range of measured flow density for | |
alpha radiation beta radiation neutron radiation: thermal neutrons, not less than intermediate and fast neutrons |
10-2 ÷ 102 cm-2s-1 10-2 ÷ 102 cm-2s-1
1 ÷ 3x103 cm-2s-1 1 ÷ 3x103 cm-2s-1 |
Ranges of measured equivalent dose rate | |
neutron radiation basal layer of the skin |
1 ÷ 1000 μSv/h 0,02 ÷ 200 μSv/h |
Spectrometric installation
SKS-99 "Sputnik"
(with the BDFI-02 detection unit)
Purpose
SKS-99 is designed for measuring the activity and specific activity of gamma-emitting radionuclides in traffic jams using the recorded spectrum of gamma quanta. SKS-99 can be used to solve problems of radiation control during the certification of food products, construction materials, forestry products, etc.
Technical characteristics
The energy ranges of the detected radiation for | |
photon radiation neutron radiation: thermal neutrons, not less than intermediate and fast neutrons |
2х102 ÷ 3x103 keV
0,4 keV 1 ÷ 1,4x104 keV |
Ranges of measured activity for | |
integral specific activity of alpha-emitting radionuclides in "thick" samples activity of gamma-emitting radionuclides in samples with the BDFI-02 detection unit (137Cs) activity surface (137Cs) |
1,5х102 ÷ 5x105 Bq/kg
8 ÷ 104 Bq 103 ÷ 106 Bq/m2 |
Ranges of measured equivalent dose rate | |
gamma radiation (with the SI-4 detection unit) |
0,1 ÷ 1000 μSv/h |
Scintillation spectrometer-radiometer of gamma and beta radiation
MKGB-01 "RADEK"
Purpose
Spectrometer-radiometer of gamma, beta and alpha radiation MKGB-01 RADEK is intended for measuring energy distribution of the gamma and beta radiation, and activity of gamma-, beta- and alpha-emitting radionuclides.
The spectrometer is stationary measurement instrument and is designed for use in the laboratory. The spectrometer is used to measure the activity (specific activity) natural radionuclides 226Ra, 232Th, 40K,222Rn, and artificial radionuclides (137Cs, 90Sr-90Y, etc.) in the soil samples, rocks, vegetation, water, food , building materials, chemical industry materials, alloys, scrap metal and other technology products. Also is used for measuring beta- and alpha- emitting radionuclides in food, biological samples and other materials.
Completeness
- Power supplies and gain units for BDEG-K
- Spectrometric beta detection units BDEB-60 (BDEB-70)
- Radiometric beta detection units BDB-60 (BDB-70)
- Radiometric alpha detection units BDA-60 (BDA-70)
- Analyzer network adapter
- Low-background chambers with shielding for units BDEG, BDEG-K, BDEB, BDB and BDA (on customer choice)
- Personal computer with software for full spectrometric analysis "ASW"
- Connecting cables
1. Area dosimetry
Laboratory work on nuclear physics is carried out using a dosimeter and a GPS navigator for coordinate binding on the locality and further construction of a radioactive contamination map.
Fig. 1: Conducting measurements of background activity of the locality and determination of the radiation dose with binding to geographic coordinates.
Fig. 2: GPS-navigator and dosimeter.
2. Dosimetry of ionizing radiation sources
Laboratory work on nuclear physics is conducted using a dosimeter and an ionizing radiation source.
Fig. 3: Device for measuring the activity of radioactive sources.
3. Spectroscopy of gamma radiation
A set of laboratory works on gamma-ray spectroscopy was developed at the International Department of Nuclear Physics, New Materials and Technologies. The complex includes the experimental plant "GAMMA-RAD5" (shown in the figure), which makes it possible to carry out experiments to study the interaction of high-energy gamma radiation with matter, as well as detecting and measuring the background of gamma radiation. Due to the peculiarities of the "GAMMA-RAD5" spectrometer construction, the whole process can be controlled by the computer to which the plant is connected. The spectrometer scintillator is wear-resistant to mechanical influences and vibrations. In addition, the device is connected via an Ethernet connection, allowing various manipulations at distances up to 100 m, or using a single USB connection for almost any computer. Finally, it has a flexible architecture that makes it possible to adapt easily the plant for specific tasks.
Fig. 4: Software package for computing gamma radiation activity.
It is worth noting that due to the above-mentioned features of the GAMMA-RAD5 spectrometer, it has a wide range of applications from laboratory measurements to the monitoring of hazardous radiopharmaceuticals in the environment and safety system.
Fig. 5: The gamma spectrometer GAMMA-RAD5, connected to the computer processing the results of gamma-radiation energy measurement.
Fig. 6: Complex of gamma spectroscopy. The graph shows the results of the gamma activity measurement of the source.
4. Laboratory of Cosmic Rays
On the basis of the International Department of Nuclear Physics, New Materials and Technologies, the Laboratory for Cosmic Ray Physics was created to measure and process helio and geophysical parameters (monitoring radiation and electromagnetic conditions). A ground-based complex of equipment has been created, including an installation for recording soft (electron-photon) and rigid (muon) components of cosmic rays. It is supposed to include a measuring instrument of electrophysical fields in the complex of ground-based instruments.
The experimental data obtained with the help of the ground complex will make it possible to carry out long-term research on such world fundamental problems of cosmophysics as:
1) Processes of acceleration of charged particles in such astrophysical objects as supernovae, the study of processes taking place on the Sun (solar flares), the propagation of cosmic rays in the near-Earth space and the magnetosphere;
2) Mechanisms and sources of modulation of cosmic ray fluxes in the interplanetary medium and heliosphere;
3) The physical role of charged particle fluxes in the terrestrial atmosphere, in global atmospheric processes (thunderstorm activity, global electrical circuit, global warming process);
4) "Space weather" on the Earth, as well as solving a number of applied problems;
5) Investigation of radiation and ionizing fields and their dynamics in the surface layer.
The laboratory uses the cosmic ray detector CARPET; they are designed for continuous monitoring of the cosmic ray flux at the Earth level.
The registration ranges of the charged particles of the counter-telescope on the basis of the gas-discharge counter STS-6:
Single counter STS-6 (channels CH1 and CH2) |
Counter telescope STS-6 (TEL channel) |
|
Electrons |
>= 0.2 MeV |
>=5 MeV |
Protons |
>= 5 MeV |
>= 30 MeV |