Thermal Analysis Mass Spectrometer Coupling. Evolved Gas Analysis Method, Techniques and Applications

Thermal Analysis Mass Spectrometer Coupling Evolved Gas Analysis Method, Techniques and Applications

Thermal Analysis and Evolved Gas Analysis Thermoanalytical Techniques Thermoanalytical techniques are universal tools for characterizing solids and liquids with respect to their thermal behavior. Especially Thermogravimetry and Simultaneous Thermal Analysis (STA, TGA-DTA/DSC) find broad application in testing the weight changes of a sample during a programmed heat treatment. This yields a multitude of information on material properties, composition and stability. However, chemical and analytical information about the products causing the weight changes to the sample is often lacking. Evolved Gas Analysis (EGA) by such techniques as quadrupole mass spectrometry can supply this additional information. Application Fields for Thermal Analysis Coupled to Mass Spectrometry QMS 43 D Aëolos Decomposition Dehydration Stability Residual solvent Pyrolysis Solid-Gas Reactions Combustion Oxidation Adsorption Desorption Catalysis Compositional Analysis Polymer content Proximate analysis Binder burnout Dewaxing Ash content Identification Gas composition Fingerprint Partial pressure Fragmentation Solid-gas interactions Evaporation Vapor pressure Sublimation 2

Reasons to Couple a Thermal Analyzer to a Mass Spectrometer Complementary Information 1 TG /% 439.2 C Ion Current *1-1 /A 3. Ion Current *1-11 /(/A) 3. DTG /(%/min) Mass changes detected by thermal analysis can be explained by gas analysis in the mass spectrometer; a workstation for analytical chemistry is thus formed. Evolved species are detected down to the ppm level, which exceeds the standard sensitivity of thermal analysis methods. The coupling of thermal analysis with mass spectrometry therefore results in high-class material research and characterization. 8 6 4 2 433.5 C m/z 14 Magnified by factor of 1 for mass no. 28 445.5 C m/z 28 1 2 3 4 5 6 7 Temperature / C 2.5 2. 1.5 1..5 2.5 2. 1.5 1..5-1 -2-3 -4-5 -6-7 Quadrupole Mass Spectrometry (QMS) 1 51 78 14 The sensitive, selective, fast and continuous functionality of a quadrupole mass spectrometer makes this system ideally suited for evolved gas analysis in combination with thermal analyzers, specifically Thermogravimetry (TGA) and Simultaneous Thermal Analysis (STA, TGA-DTA/DSC). 5 1 34 39 44 56 63 65 74 83 89 91 98 11 115 123 13 134 139 168 183 198 29 143 152 164 179 187 194 22 44 54 64 74 84 94 14 114 124 134 144 154 164 174 184 194 24 14 MS spectrum at 439.2 C Optimum coupling with thermal analyzers is provided thanks to the small dimensions of the quadrupole mass filter, the efficient and reproducible ionization of gases in the electron impact ion source, and the resolution in the detection of molecules, atoms and fragments. 5 34 39 41 51 63 74 65 78 84 89 98 44 54 64 74 84 94 14 114 124 134 144 154 164 174 184 194 24 Upper plot: TGA-QMS Aëolos measurement on an unknown polymer shows one mass-loss step between 4 C and 46 C. Lower plot: NIST library search of the spectrum measured at 22.4 min clearly indicates styrene. Also the dimer of styrene is detected, see mass number 28 in the upper plot. 3

HYPHENATION OF THERMAL ANALYSIS AND EVOLVED GAS ANALYSIS STA 449 F1 Jupiter coupled to QMS 43 D Aëolos ; other thermal analyzers can also be coupled to MS, such as the TG 29 F1 Libra 4

Withstanding the Test of Time Capillary and SKIMMER Coupling Techniques NETZSCH offers complete solutions for Thermal Analysis coupled to Mass Spectrometry in terms of both hardware and software. Evaluation and presentation of the results is carried out with the well-proven Proteus software. Gas flow conditions in all thermal analyzers are ideal for coupling to a mass spectrometer via capillary or a double-orifice system known as the SKIMMER coupling. By measuring the mass numbers (m/z), conclusions on the composition of the evolved gases can be drawn. While the capillary coupling is well-suited for the investigation of permanent gases, the SKIMMER coupling is advantageous for metallic ions and inorganics where condensation can be expected at higher temperature. STA 49 CD SKIMMER 5

TA-QMS Coupling Techniques Interface for Pressure Adjustment Mass spectrometers, composed of a mass filter, an electron impact ion source and an ion detector, work only in high vacuum. Therefore, an interface is required for the coupling of a thermobalance which works with a purge gas flow at atmospheric pressure to the mass spectrometer. Different versions of pressure reduction interfaces are realized, depending on instrumentation and applications. QMS 43 D Aëolos Single-Step Pressure Reduction A capillary of small internal diameter connects the gas outlet on the furnace of the thermobalance with the gas inlet on the mass spectrometer. The pressure drops from atmospheric pressure down to high vacuum in one continuous step. STA 49 CD SKIMMER Double-Step Pressure Reduction Different systems such as laminar flow capillary, nozzle, and orifice are used to reduce the pressure in the first step down to the range from 1-1 mbar to 1 mbar. A membrane pump, rotary pump or the drag stage of the turbo molecular pump is applied to achieve this pressure reduction. The second step is either an orifice or a skimmer as a molecular leak for the gas inlet into the high-vacuum recipient of the mass spectrometer. Step 1 Pump Step 2 1 3 mbar 1-5 mbar Pump 1 3 mbar 1-5 mbar Pump Interface Interface Thermobalance Mass Spectrometer Thermobalance Mass Spectrometer Capillary Coupling Double orifice SKIMMER coupling 6

Ideal Gas Flow Conditions Ensure Transport of All Relevant Gases The aim of coupling is to have all relevant gases and vapors transported from the sample area into the ion source of the mass spectrometer for precise qualitative and quantitative analysis. This is only achieved through perfect gas flow conditions in the thermal analyzer, the coupling interface and the gas inlet of the mass spectrometer. As only a small quantity of gas is required for the analysis, a bypass is used at the gas outlet on the thermobalance for the excess purge gas flow; i.e., for the flow not passing through the coupling interface, which can be used for a second gas analyzer such as FT-IR. QMS 43 D Aëolos QMS transfer line 25 C to 3 C Gas outlet and FT-IR connection 25 C to 23 C Quadrupole analyzer 1-5 mbar Ion source Coupling adaptor 25 C to 3 C 1-1 mbar Capillary Skimmer Orifice Sample Heater Sample carrier 113 mbar Gas overflow Capillary coupling Double orifice SKIMMER coupling Perfectly coupled for precise results. 7

Coupling TA-QMS 43 D Aëolos A fleshed-out design for capillary coupling to NETZSCH thermal analyzers (e.g., simultaneous TGA-DSC, STA) can be found in the QMS 43 D Aëolos quadrupole mass spectrometer. Volatile sample materials under a controlled temperature treatment are directly transferred into the electron impact ion source of the MS via a fused silica capillary. TOP-LINE CAPILLARY COUPLING Overall Heating and Single-Step Pressure Reduction The Capillary Coupling is Designed for Optimum Gas Flow Conditions and Flexibility Minimization of cold spots in the transfer path Minimized condensation losses due to overall temperature of 3 C across the entire gas transfer system from the furnace outlet to the capillary to the MS gas inlet. Flexible, allowing standard thermoanalytical measurements and also simultaneous TGA, MS (GC-MS) and MS-FT-IR measurements. Very robust and service-friendly while still maintaining high sensitivity (detectable mass loss in the μg-range). Allows TGA-MS measurements under humid atmospheres. Upgrade of existing thermal analyzers. The QMS 43 D Aëolos can also be independently employed for the analysis of other gas sources. TGA-DSC/DTA Systems STA 449 F1 Jupiter T-range: -15 C to 2 C Weighing range: 5 g TGA resolution:.25 μg STA 449 F3 Jupiter T-range: -15 C to 24 C Weighing range: 35 g TGA resolution:.1 μg STA 449 F5 Jupiter T-range: RT to 16 C Weighing range: 35 g TGA resolution:.1 μg TGA Systems TG 29 F1 Libra T-range: RT to 11 C Weighing range: 2 g TGA resolution:.1 μg Automatic sample changer for up to 192 sample pans 8

Insulated inert quartz glass capillary with controlled heating to 3 C for lossfree gas transfer to the QMS Heated chamber for easy handling and precise adjustment of the capillary inlet to the QMS Natural vertical gas flow through the STA furnace to the heated adapter with capillary inlet and bypass Quadrupole MS with cathode, electron and ion lenses, mass filter and Channeltron detector DSC/DTA Systems DSC 44 F1/F3 Pegasus T-range: -15 C to 2 C High-sensitivity and highresolution sensors Dilatometer/Thermomechanical Analyzer DIL 42 Supreme T-range: -18 C to 2 C Measuring range: 5 μm Δl resolution:.1 nm DIL 42 Select T-range: -18 C to 16 C Measuring range: 2 μm Δl resolution: 1 nm TMA 42 F1/F3 Hyperion T-range: -15 C to 155 C Measuring range: 5 μm/5 μm Δl resolution:.125 nm/1.25 nm 9

Continuous heating of the entire gas transfer line reduces the risk of condensation so that even larger molecules can be detected.. -1. -2. -3. -4. -5. 1 5 TG /mg 264.3 C 27.1 C 5 1 15 2 25 3 35 4 45 Temperature / C 55 57 71 85 Ion Current DTG *1-9 /A /(mg/min) 5. 99 113 24 67 127 45 77 91 141 155 169 183 197 21 4 5 6 7 8 9 1 11 12 13 14 15 16 17 18 19 2 21 22 23 24 25 1 57 5 43 71 85 NIST Spectrum 4 3 2 1 -.5-1. -1.5-2. -2.5-3. -3.5 Optimized Transfer Path Allows for the Detection of Larger Molecules Heptadecane Detection This measurement was carried out with the STA 449 F3 Jupiter coupled to the QMS Aëolos. The temperature adapter, transfer line and MS inlet were set to 3 C. Evaporation of this unbranched isomer (CH 3 (CH 2 ) 15 CH 3 ; bp. 32 C) starts at approx. 17 C (blue curve). The maximum decomposition rate is achieved at 264,3 C (DTG peak, dotted line) when using a heating rate of 2 K/min. After a short delay (.4 min), the ion current achieves its maximum at 27,1 C (dark blue curve). After detection of heptadecane in the MS, the ion current immediately returns to the zero-level without any tailing effect. A comparison between the detected MS spectrum for heptadecane and the corresponding NIST library spectrum confirms that even larger molecules (e.g., m/z 24) pass the adapter, transfer line and MS inlet without condensation. 41 55 99 113 91 15 119 127 133 141 145 155 169 183 197 211 24 45 77 4 5 6 7 8 9 1 11 12 13 14 15 16 17 18 19 2 21 22 23 24 25 1

ACCESSORIES MAKE THE DIFFERENCE Water-Vapor Furnace up to High Water-Vapor Concentrations STA-MS Measurements under Water-Vapor Atmosphere Furnace In addition to a variety of other furnaces for the STA systems, NETZSCH also offers a watervapor furnace which allows for pure vapor atmospheres at the sample between room temperature and 125 C. The watervapor furnace can be connected with a humidity or a watervapor generator. It provides protection against flooding and minimal dilution due to a special gas flow design. Sample chamber Heated transfer line from vapor generator Water vapor carrier gas protective gas Heated transfer line to Aëolos Heated Aëolos adaptor Outlet Monitoring Reaction Steps During the Carbon Gasification Process This plot shows a typical example of the configuration with the water-vapor furnace: Here, the water vapor present in relatively high concentrations (2% H 2 O) serves as a reactant for the transition from coal to hydrogen, and the STA with coupled gas analysis shows both the weight loss of the coal sample and the products resulting from the reaction. 12 1 TG /% 8 6 4-2.5 % -1.8 % -6.8 % -3.4 % switching to Ar+2% H2O carbon gasification: C + H 2 O CO + H 2 CO + H 2 O CO 2 + H 2 2 amu 28 (CO) decomposition of organics amu 44 (CO2) amu 2 (H2) -2 1 2 3 4 5 6 7 8 9 Time /min Ion Current *1-1 /A 8 6 4 2 Tem. / C 8 7 6 5 4 3 2 1 11

TA-QMS 43 D Aëolos Application Measurement of an Unknown Polymer This TGA-MS measurement of an unknown polymer (7.52 mg) was carried out in the temperature range between room temperature and 25 C in a helium atmosphere. The 3-D plot above shows the TGA measurement together with the MS results. The plot on the right correlates the TGA curve with various MS traces of m/z 35, 47, 48, 51, 77, 83, and 15. By exporting the 2-dimensional scan-bargraph directly into the NIST database (see image below as an example at 166 C), it becomes possible to interpret the individual mass-loss steps. TG /% Ion Current *1-12 /A Ion Current *E-12 /A 4 3 2 1 4 5 6 7 m/z 8 9 1 11 5 1 4 35 3 25 2 15 Temperature / C 1 9 8 7 6 5 4 3 2 1 amu 35 amu 44 amu 47 amu 48 amu 51 amu 77 amu 81 amu 83 amu 15 5 1-9.4 % -1.71 % 5. -3.85 % 4. 191. C 3. 172.7 C 247.5 C 241.8 C 2. 166.4 C 189.7 C 1. 15 2 25 Temperature / C 3-D plot of a TGA-MS measurement on an unknown polymer sample as a function of temperature Correlation of mass-loss steps and different gases detected and identified in the MS; 35 amu most probably corresponds to HCl. 12

Direct export of the MS results at 166 C into the NIST database for identification of the evolved gases 13

SKIMMER DOUBLE ORIFICE SOLUTION FOR HIGH-BOILING MATERIALS DETECTION OF Large molecules Highly condensable (metal) vapors Permanent gases Vertical Top-Loading STA System and SKIMMER on Top of the Furnace The SKIMMER coupling (realized with the STA 49 CD) actualizes the shortest possible route for gas transfer from the sample to the QMS. The SKIMMER collimates the molecules from the barrel-shaped jet expansion behind the divergent nozzle towards the QMS ion source. The pressure reduction of the purge gas flow from atmospheric pressure down to the high vacuum behind the SKIMMER orifice is achieved in two steps along a distance of less than 2 mm. This drastically reduces the risk of condensation and thus achieves high detection sensitivity. Even metal vapors are detected by this unrivaled coupling system. The nozzle and SKIMMER are precisely machined from either alumina or glassy carbon, allowing application temperatures of 145 C or 2 C in the corresponding furnaces. The molecular beams are analyzed by a quadrupole mass spectrometer up to high mass numbers of 512 u or optionally 124 u. Detection of Metal Vapors Lead chloride (7.92 mg) in an argon flow of 15 ml/min exhibits evaporation starting in the melting range (487 C). The molecule ion (PbCl 2 m/z 278) and fragment ions caused by dissociation and ionization (PbCl m/z = 243, Pb m/z = 28, Cl m/z 37, Cl m/z = 35) are clearly detected far below the boiling temperature of the starting material. 1 TG /% 8 6 4 2 TG DSC MID 487.3 C 4 45 5 55 6 65 7 75 8 85 Temperature / C 35 37 699. C 28 73.1 C 278-97.1 % 243 exo -2.9 % DSC /uv 25 2 15 1 5-5 -1 Ion Current *1-11 /A 3.5 3. 2.5 2. 1.5 1..5 14

Quadrupole MS Intermediate vaccuum SKIMMER Supersonic jet expansion zone Divergent nozzle Sample Furnace Sample holder Gas overflow capillary Shortest possible coupling solution via unique supersonic jet gas transfer 15

SKIMMER Applications Thermal Stability of the Thermoelectric Material PbTe PbTe Isotopes (m/z) Pb und Te Isotopes Knowledge about thermal stability properties, such as phase change and evolving gases at elevated temperatures, is crucial for the development of thermoelectric materials. In this example, the thermal stability of PbTe was analyzed using the STA 49 CD coupled to a mass spectrometer via the SKIMMER system. The plots each show the TGA curve of the PbTe sample, but with different mass spectrometer results. PbTe starts decomposing at around 6 C. The plotted mass numbers represent the combination of the Pb and Te isotopes. The following gaseous products were detected: 332 u 27 Pb + 125 Te 26 Pb + 126 Te 333 u 28 Pb + 125 Te 27 Pb + 126 Te 334 u 28 Pb + 126 Te 26 Pb + 128 Te 335 u 27 Pb + 128 Te 336 u 28 Pb + 128 Te 337 u 27 Pb + 13 Te 338 u 28 Pb + 13 Te TG /mg Ion Current *1-12 /A TG /mg Ion Current *1-12 /A -1-2 -3-4 -5-6 PbTe.23455E-9A*s.28191E-9A*s 332 333-6.43 mg 1.2 1..8.6.4.2-1 -2-3 -4-5 -6 PbTe.2489E-9A*s.19645E-9A*s 335 337-6.43 mg 1..8.6.4.2 2 4 6 8 1 12 Temperature / C 2 4 6 8 1 12 Temperature / C TG /mg Ion Current *1-12 /A TG /mg Ion Current *1-12 /A -1-2 -3-4 -5-6 PbTe.5277E-9A*s.532E-9A*s 334 338-6.43 mg 2.5 2. 1.5 1..5-1 -2-3 -4-5 -6 PbTe.71867E-9A*s.5572E-9A*s 336 338-6.43 mg 3.5 3. 2.5 2. 1.5 1..5 2 4 6 8 1 12 Temperature / C 2 4 6 8 1 12 Temperature / C 16

Sophisticated applications require ingenious analytical tools Decomposition Products of Carbon Pitch TG /% 1 TG Ion Current *1-1 /A 2.5 Carbon pitch is the primary product from the distillation of coal tar. It is used as a binding agent in the production of carbon anodes for aluminum smelters and graphite electrodes for electric arc furnace steel producers. 95 9 85 8 DTG 322. C 22-8.67 % -6.3 % 252 535.3 C -3.18 % 2. 1.5 1. Carbon pitch powder (55.2 mg) decomposes in a nitrogen flow (5 ml/min) into aromatic compounds of high molecular weight, mainly below 6 C. Only a selection is shown here with MID curves for such substances as pyrenes (m/z = 22), triphenylenes m/z = 228), benzo(a)pyrenes (m/z = 252), benzo(ghi)perylenes (m/z = 276) and dibenzopyrenes (m/z = 32). 75 7 MID 228 276 32 2 4 6 8 1 12 Temperature / C.5 Detection of aromatic compounds of high molecular weight 17

PulseTA Calibration/Quantification The quantification of MS signals requires calibration of the whole coupled system with a known type and amount of gas or solvent to control for the temperature-dependent flow properties. PulseTA is a perfect tool for achieving quantitative gas detection in separate calibration runs or even online during a sample measurement. A known amount of gas is injected into the sample gas stream and the registered signal of the resulting pulse is integrated. The application of PulseTA also allows for studying gas/solid reactions with stepwise control of the process via the injection of a reactive gas, and simplifies adsorption/desorption experiments. injected Injected gas carrier Purge gas TA MS/FT-IR MS/FTIR pulse Pulse device TGA-DSC Gas composition Inert gas CO 2 pulses for calibration of a carbonate decomposition Reactive gas (gas-solid reaction) Reduction of metal oxide by H 2 pulses Reactive gas (adsorption) NH 3 adsorption by a zeolithe sample CO 2 TG TG H 2 m/z = 44 NH 3 18

Quantification of Contaminations on an Mo Wire Separation of Overlapping Oxidation and Carbon Burn-Up TG /% 11 1.8 1.6 1.4 1.2 1. 99.8 amu 44 (CO 2 ) 473. C -.2% 56.6 C 1 2 3 4 5 6 7 Temperature / C Heating of a molybdenum sample (4153.9 mg) in an Al 2 O 3 beaker at a heating rate of 1 K/min in a synthetic air atmosphere. The sensitivity of the QMS 43 D Aëolos is linear and temperature-independent. Ion Current *1-9 /A.85% 1.5 1..5 -.5 In this analysis, a small mass loss of.2% occurred below ~5 C, followed by an increase in sample mass of.85% due to oxidation of the sample. At the same time, carbon impurities on the wire s surface were burnt, which can be seen from the MS signal for m/z 44 due to the CO 2 release (solid line). The carbon content was quantified at ~9 ppm by means of the NETZSCH PulseTA device as follows: During an empty run, several CO 2 pulses of defined volumes (.25 ml and 1 ml) were injected into the STA and detected by the MS (dashed line). From the ratio of the ion current peak areas of the calibration pulses and the signal from the sample, the amount of CO 2 evolved from the sample can be calculated. 19

Proteus Software for TA-MS Coupling The control of measurements with coupled TGA-QMS instruments is governed by the Proteus software. The user gives the command for data acquisition once both the QMS and the Proteus software are ready with parameter inputs as well as checked pressure and ion source conditions. The online data collection is simultaneous and synchronized through a triggered start to guarantee precise time and temperature correlation among all the signals from the two systems during evaluation. The user works with the two software packages on one computer and has access to the entire spectrum of possibilities for evaluating data and displaying results in the Proteus software according to preference. The integration of the TA and QMS software based on effective data exchange from acquisition to evaluation is what makes the coupled TGA-QMS to a true functional unit. 2

Key Software Features Direct import for MS data Evaluation of MS data within Proteus Simultaneous start/stop of the coupled measurements (trigger system) Evaluation of results precisely correlated in terms of time and temperature Integration of MS peaks (MID and QMID peaks) Fast MID input of 8 mass numbers Several scan-bargraph ranges with fast mass range input Selection of up to 64 MID mass numbers Selection of analog scans in max. 64 channels Selection of scan-bargraphs or scan analog graphs with optimized rate and sensitivity in 4 different channels Spectra export in NIST format for identification in the NIST database TGA-DSC/DTA total ion current 3-D presentation of spectra data together with temperature, TGA and/or DSC curves, including peak determination (see plot on the left) Navigator to enlarge, reduce or rotate the 3-D plot (see plot on the left) Turbo pump and pressure displayed by software TGA-DSC/DTA-MID curves and scan-bargraph envelope curves: characteristic temperatures, peak areas 21

Various Ways of Presenting Test Results for Optimum Evaluation 1,E-6 Comprehensive Information via Scan-Bargraph Ion Current/A 1,E-8 1,E-1 1,E-12 1 15 2 25 3 35 4 45 5 55 6 65 7 Mass/Charge A scan-bargraph is often the basis for depicting comprehensive information about all of a sample s evolved species; it allows for the selection of all mass numbers or just individual ones of interest for import into the Proteus software as continuous MID curves. Here, one scan out of the repeated scans is shown for Nd 2 (SO 4 ) 3 5 H 2 O measured in air at 95 C. TG /% 1 9-12.7% Ion Current *1-9 /A 4. 3.5 Direct Correlation Between Mass Loss and Evolved Gas via MID Curves 8 7 6 5 amu 18 (H 2 O) amu 32 (O 2 ) -23.61% amu 64 (SO 2 ) -11.79 % 3. 2.5 2. 1.5 1..5 Nd 2 (SO 4 ) 3 4.7 H 2 O (29.53 mg) was heated at a rate of 1 K/min up to 14 C in a nitrogen flow. The MID curves, directly imported from the coupled Aëolos, show the well separated gas evolution for water, oxygen and sulfur dioxide in perfect correlation with the TGA steps. 4 2 4 6 8 1 12 14 Temperature / C 22

Key Technical Data QMS 43 D Aëolos QMS mass range 3 u* Resolution >.5 u* Scan, Scan-Bargraph, MID Electron impact ionization Ionization energy: 25 ev to 1 ev Two iridium cathodes, Y 2 O 3 -coated Channeltron SEM Single-step pressure reduction Detection limit 1 ppm 1 3 mbar to 1-5 mbar Turbo molecular and membrane pump systems (oil-free) Quartz glass capillary Insulated; Ø 75 μm; length 2.5 m Entire transfer heated at 3 C * u: unified atomic mass STA 49 CD with SKIMMER RT to 145 C, SiC furnace Temperature range RT to 2 C, graphite furnace Weighing range 15 g TGA resolution 2 μg Sensor types TGA, DSC, DTA Alumina (up to 145 C) SKIMMER systems Glassy carbon (up to 2 C) QMS QMS options 1 to 512 u 1 to 124 u Analog scan, scanbargraph, Measuring modes MID Ion source Cathodes Detection limit Electron impact ionization: Energy up to 125 ev; adjustable in steps of 1 ev Tungsten; others on request < 1 ppb 23

The NETZSCH Group is a mid-sized, family-owned German company engaging in the manufacture of machinery and instrumentation with worldwide production, sales, and service branches. The three Business Units Analyzing & Testing, Grinding & Dispersing and Pumps & Systems provide tailored solutions for highest-level needs. Over 3,4 employees at 21 sales and production centers in 35 countries across the globe guarantee that expert service is never far from our customers. When it comes to Thermal Analysis, Calorimetry (adiabatic & reaction) and the determination of Thermophysical Properties, NETZSCH has it covered. Our 5 years of applications experience, broad state-of-the-art product line and comprehensive service offerings ensure that our solutions will not only meet your every requirement but also exceed your every expectation. NETZSCH-Gerätebau GmbH Wittelsbacherstraße 42 951 Selb Germany Tel.: +49 9287 881- Fax: +49 9287 881 55 at@netzsch.com NGB Thermal Analysis Mass Spectrometer Coupling EN 517 NWS Technical specifications are subject to change.