In the week of July 13, the following webinars await you in the field of gas / solid phase and especially Raman, FTIR, GC and GC/MS.<blockquote><h4><a target="_blank" rel="noopener noreferrer" href="https://gcms.labrulez.com/webinars">👉 DETAILS AND REGISTRATION IN THE WEBINARS SECTION</a></h4>👉 Search and filter in the largest global database with over 5 500 GC, LC, MS and spectroscopy webinars.</blockquote><h5>1. Markes International: Understand the aromas consumers really experience</h5><ul><li>Tu, 14.7.2026 10:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://gcms.labrulez.com/webinar/6382">Registration</a></li></ul>Join Markes as they unveil their latest innovation and explore a new approach to helping researchers and product developers gain a deeper understanding of aroma evolution.<h5>2. Thermo Fisher Scientific: Helium, PFAS &amp; Recycled Plastics: Addressing Key Challenges in Industrial Laboratories</h5><ul><li>Th, 16.7.2026 08:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://gcms.labrulez.com/webinar/6337">Registration</a></li></ul>Tackle industrial GC challenges. Learn strategies for helium conservation, PFAS testing using TD-GC-MS, and analytical solutions for recycled plastics.<h5>3. C&amp;EN: Microplastics Analysis You Can Defend: From Method to Results</h5><ul><li>Th, 16.7.2026 11:00 CEST</li><li><a target="_blank" rel="noopener noreferrer" href="https://gcms.labrulez.com/webinar/6334">Registration</a></li></ul>Strengthen your microplastics analysis. Learn how combining LDIR chemical imaging and pyrolysis-GC/MS improves data quality across complex sample matrices.

Webinars LabRulezGCMS Week 29/2026

This study optimizes the quantification of hydrogen point-source emissions through controlled-release experiments using an 8 kW electrolyzer. A multiplatform AirCore sampling system coupled with a high-resolution GC-PDHID simultaneously measured hydrogen, methane, and carbon dioxide to evaluate how sampling conditions influence emission estimates.Analysis of UAV and ground-based measurements showed that plume coverage, wind variability, and sampling resolution strongly affect emission accuracy. The results also demonstrated that hydrogen plume behavior closely resembles methane, indicating that established methane monitoring strategies can be adapted for hydrogen leak detection and supporting future assessments of hydrogen as an indirect greenhouse gas.<blockquote><h4>The original article</h4><h4><a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/10.1021/acsestair.6c00006">Controlled-Release Experiment to Optimize Emission Quantification of H2 Point Sources</a></h4>Iris M. Westra*, Hubertus A. Scheeren, Mareen J. Penninga, Steven M.A.C. van Heuven, and Harro A.J. MeijerACS EST Air 2026, 3, 6, 1576–1585<a target="_blank" rel="noopener noreferrer" href="https://doi.org/10.1021/acsestair.6c00006">https://doi.org/10.1021/acsestair.6c00006</a><h6>licensed under <a target="_blank" rel="noopener noreferrer" href="https://creativecommons.org/licenses/by/4.0/">CC-BY 4.0</a></h6></blockquote>Selected sections from the article follow. Formats and hyperlinks were adapted from the original.<div>Currently, more than 90% of hydrogen produced is gray hydrogen, derived primarily from steam methane reforming or coal gasification, both of which are carbon-intensive. <a href="javascript:void(0);">(1)</a> Considering the global hydrogen budget, the primary natural source of atmospheric hydrogen is sunlight-driven production (e.g., via methane oxidation), contributing 38 ± 6 Tg yr–1 (about 55% of the total budget). The largest anthropogenic source of hydrogen is the combined contribution from biofuel burning and wildfires, amounting to 12 ± 4 Tg yr–1. <a href="javascript:void(0);">(1)</a> Hydrogen’s indirect Global Warming Potential (GWP) leads to the lengthening of the lifetime of CH4 and ozone, and to increased levels of stratospheric water vapor (H2O). <a href="javascript:void(0);">(2,3)</a> As a result, the GWP of H2 over a 100-year time scale has been estimated at 11.6 ± 2.8, indicating that H2 is 12 times more potent than CO2. <a href="javascript:void(0);">(4)</a> While this is about half the GWP of CH4 it underscores the significance of hydrogen’s indirect effects on climate when released into the atmosphere. <a href="javascript:void(0);">(5)</a> Until recently, small but climate-relevant hydrogen emissions remained undetected along the entire hydrogen value chain. However, such hydrogen losses during production, transport, storage and consumption could lead to a greater atmospheric hydrogen burden. <a href="javascript:void(0);">(3)</a> To illustrate the impact of hydrogen leakage, the HC2017 scenario presented in Hauglustaine et al. (2022) shows that, for a hydrogen mix of 30% blue (gray+CCS) and 70% green hydrogen (renewables) with leakage rates of 1–3%, the climate benefit is substantially reduced, with hydrogen CO2-equivalent emissions corresponding to 20 to 54% of the avoided CO2 (based on GWP100 and GWP20, respectively). At higher leakage rates (&gt;10% for a 100-year horizon; &gt; 5% for a 20-year horizon), this hydrogen mix results even in a net climate penalty, where CO2-eq emissions exceed the avoided CO2.Thus, far, current loss rate estimates, ranging up to 10%, are solely based on bottom-up emission estimates (i.e., theory-based). <a href="javascript:void(0);">(6−8)</a> A limited amount of suitable measurement equipment and a current lack in actual measurements causes these estimates to have no validation. <a href="javascript:void(0);">(9)</a>Only recently, sensitive new techniques to detect low-level hydrogen emissions along the value chain on an atmospheric scale have become available. In our previous study <a href="javascript:void(0);">(10)</a> we combined an established high-precision analysis method (gas chromatograph─pulsed discharge helium ionization detector; GC-PDHID) with a newly applied sampling method (active AirCore <a href="javascript:void(0);">(11)</a>) deployed from various mobile platforms, to detect significant hydrogen emissions originating from a chemistry park in the Netherlands. <a href="javascript:void(0);">(10)</a> In the meantime, Aerodyne Research Inc. (USA) has developed a laser-spectroscopy-based instrument with which atmospheric hydrogen can be measured continuously, through oxidation to water vapor and a subsequent optical measurement, achieving ∼5 ppb precision (per 5 s). <a href="javascript:void(0);">(12,13)</a> The Norwegian oil company Equinor, in collaboration with Advanced Monitoring Solutions (AdMS) and the Department of Chemistry (University of Oslo) in Norway, have developed a mass spectrometer system capable of measuring small atmospheric hydrogen mole fractions (&lt;1 umol mol–1 i.e., ppm) with a detection limit of ∼10 nmol mol–1 (i.e., ppb) directly from dried ambient air. <a href="javascript:void(0);">(14)</a> Hence, with these new developments in atmospheric hydrogen detection techniques, the hitherto unknown hydrogen emissions along the hydrogen value chain become visible.In the field of emission quantification there is already a wealth of reported experiments for greenhouse gases (GHG), like methane (CH4), <a href="javascript:void(0);">(15)</a> with the aim of making emission quantifications more reliable and accurate. These emission estimates help reduce uncertainties in bottom-up estimates of the greenhouse gas (GHG) budget. <a href="javascript:void(0);">(16)</a>Optimal airborne plume sampling for methane emissions from a point source depends on factors such as the downwind distance, maximum flight time, measurement precision, and atmospheric stability conditions. <a href="javascript:void(0);">(17)</a> Especially during near-source sampling (&lt;500 m downwind), accurate visualization of the plume in both the horizontal (width) and vertical (height) plane is critical for reducing significant discrepancies between measured emissions and inventory estimates. <a href="javascript:void(0);">(18−20)</a> Furthermore, Morales et al. showed that measurement uncertainties increase primarily under conditions of wind speeds below 2 m s–1, wind direction variability greater than 33°, and sampling at downwind distances greater than 75 m. So far, under the most favorable measurement conditions, CH4 emissions could be quantified with an overall uncertainty of at best 30%. <a href="javascript:void(0);">(17)</a>In this study, we use measurements from a controlled-release experiment to optimize the quantification of hydrogen point-source emissions by identifying the most influential parameters contributing to uncertainties in the emission estimates.In the following, we first outline the sampling and analysis techniques, building on Westra et al., <a href="javascript:void(0);">(10)</a> after which we give a site description and further necessary prior information. The observations obtained from ground-based and airborne measurements are analyzed using a Gaussian plume dispersion model combined with a Monte Carlo uncertainty analysis to estimate the emission rate. At the end of the paper the conclusions and outlook on our methodology will be given.<h4>2. Materials and Methods</h4><h5>2.4. Analysis Methods</h5>The <a target="_blank" rel="noopener noreferrer" href="https://gcms.labrulez.com/library?mainauthorItems=10&amp;search=8890">Agilent 8890 gas chromatograph</a> pulsed discharged helium ionization detector (GC-PDHID) system setup was designed for the precise and accurate analysis of H2, CO2 and CH4 in dry ambient air. We chose a PDHID for its high sensitivity, reliability, and good linearity from low to high mole fractions for H2 (here typically ranging between 0.5 up to 5 ppm). The system setup enables, via a heart-cutting procedure (forward-flush mode of the O2 and N2 fraction), the simultaneous detection of CO2 and CH4, which can aid in the source apportionment of atmospheric H2.Our system design was partly based on the Agilent setup 7890–0237 “Impurities in Monomers Analyzer by PDHID” and a GC setup by Wang et al. <a href="javascript:void(0);">(24)</a> The PDHID system uses Helium 5.0 (99.9999% Vol. %, Westfalen) as carrier gas, for a combination of a HayeSep Q, (G3591–81004, 6 ft,18” “, 2 mm, 80–100 mesh packed) pre-column, followed by a ShinCarbon (G3591–81187, 2 m, 18”, 2 mm, 50/80 mesh) analytical column for detection of H2, CH4 and CO2. For the sample analysis a 2 mL sample loop is flushed at a rate of 43 ± 2 mL min–1 for 0.01–0.67 min. One chromatogram lasts 15.5 min for the detection cycle of H2, CH4 and CO2, and 7.5 min for H2 only. Retention times for the H2–CH4–CO2-method are 2.8 ± 0.1 min for H2 with a 4.2 ± 1.0 s wide peak width (PW), 7.7 ± 0.1 min for CH4 with a 16.8 ± 1 s PW, and 13.9 ± 0.1 min for CO2 with a 78 ± 1 s PW, and for the single H2-method at 2.3 ± 0.1 min for H2 with a 4.8 ± 1.0 s PW. A more detailed description of the GC analysis is given in <a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/suppl/10.1021/acsestair.6c00006/suppl_file/ea6c00006_si_001.pdf">Section S1.1</a>.<h4>3. Results and Discussion</h4><h5>3.2. AirCore Results</h5>The determined emission rates were achieved by applying the Gaussian dispersion model to the found H2 enhancements for each transect, and by taking into account the atmospheric conditions during sampling, following the approach outlined in Westra et al. <a href="javascript:void(0);">(10)</a> Using an 8 kW electrolyzer (<a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/10.1021/acsestair.6c00006#fig4">Figure 4</a>) with a known, continuous release rate of 1.1 ± 0.1 m3 h–1 as a controlled source, we analyzed 14 data sets to determine a mean weighted hydrogen emission rate of 0.94 ± 0.06 m3 h–1. This agrees well within uncertainty with the known source rate. The relative uncertainty (ratio of uncertainty over average) of the emission estimate is 6%, compared to 9% for the known source. The source-based uncertainty was derived from variability in the electrolyzer exhaust monitored over multiple hours. More information with regard to the uncertainty analysis can be found S1.5. All data gathered during the field experiments is given in <a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/suppl/10.1021/acsestair.6c00006/suppl_file/ea6c00006_si_001.pdf">Sections S2.1 and S2.4</a>.<img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/ACS_EST_Air_2026_3_6_1576_1585_Figure_4_Emission_rates_estimated_for_six_sampling_days_using_the_Gaussian_dispersion_model_and_the_Air_Core_technique_a84e3bb1b0.jpg" alt="ACS EST Air 2026, 3, 6, 1576–1585: Figure 4. Emission rates estimated for six sampling days using the Gaussian dispersion model and the AirCore technique, measured downwind of the electrolyzer at varying distances. Measurements were conducted either at ground level (cart icon) or via UAV (drone icon). Boxplots represent results from 500 Monte Carlo simulations, displaying the mean and interquartile range. From 28 to 11–2024 onward the, as described, an optimized sampling method was used." srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_ACS_EST_Air_2026_3_6_1576_1585_Figure_4_Emission_rates_estimated_for_six_sampling_days_using_the_Gaussian_dispersion_model_and_the_Air_Core_technique_a84e3bb1b0.jpg 234w," sizes="100vw" width="1453" height="970">On day 13–11–2024, the quality of the data collected along the first 100 m trajectory was lower due to a sampling flow rate of ∼45 sccm combined with a relatively high rate of displacement. As a result, the full plume width was not captured, and the spatial resolution of the measurements was insufficient. This limitation, consistent with the findings of Mohammadloo et al., <a href="javascript:void(0);">(15)</a> led to the underestimation of the actual emission rate. Particularly for transect 100 m (1), where the plateau-shaped peak approximated a Gaussian peak, led the dispersion model to substantially underestimate the emission rate (<a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/suppl/10.1021/acsestair.6c00006/suppl_file/ea6c00006_si_001.pdf">Sections S1.6 and S2.3</a>). Furthermore, the relatively large spread in data points observed throughout the remaining trajectories of 13–11–2024 can be attributed to the sampling time of the experiment, during which the atmospheric variability (i.e., wind speed and direction) impacted the uncertainty. As a result, the Monte Carlo simulations produced a wider range of solutions due to this variability, and thus a greater spread in the values. So, the impact of the atmospheric conditions could be reduced by minimizing sampling time and thereby reducing the atmospheric variability.For day 14–11–2024 (<a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/10.1021/acsestair.6c00006#fig5">Figure 5</a>), an average wind speed of 1.7 ± 1 m s–1 was measured. According to Andersen, <a href="javascript:void(0);">(22)</a> wind speeds below 2 m s–1 lead to ill-defined wind directions, making the plume less likely to follow a stable path and thereby increasing uncertainty in the emission estimate. Hence, it is likely that the lower wind speed on this day contributed to less reliable results in the emission quantification. Moreover, for day 14–11–2024, the wider spread observed in the estimates (<a target="_blank" rel="noopener noreferrer" href="https://pubs.acs.org/doi/10.1021/acsestair.6c00006#fig4">Figure 4</a>) is attributed to incomplete coverage of the plume width along the 100 m downwind transects.<img src="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/ACS_EST_Air_2026_3_6_1576_1585_Figure_5_Trajectory_of_ground_based_Air_Core_profile_downwind_of_the_electrolyzer_2f1d50dfd7.jpg" alt="ACS EST Air 2026, 3, 6, 1576–1585: Figure 5. Trajectory of ground-based AirCore profile downwind of the electrolyzer (shown by the “x”) on 14–11–2024, first round (a, b) and second round (c, d), shown on a 300 m scale and the H2 mole fraction (ppb) given in the legend on the right. The total sampling time of the trajectory was 35 min. Map tiles © Mapbox, data © OpenStreetMap contributors (ODbL), modified by the author." srcset="https://storage.googleapis.com/labrulez-bucket-strapi-h3hsga3/thumbnail_ACS_EST_Air_2026_3_6_1576_1585_Figure_5_Trajectory_of_ground_based_Air_Core_profile_downwind_of_the_electrolyzer_2f1d50dfd7.jpg 184w," sizes="100vw" width="1627" height="1383"></div>

Controlled-Release Experiment to Optimize Emission Quantification of H2 Point Sources

A Rapid, Antigen-Independent Diagnostic Strategy for Chronic Chagas Disease Based on Serum ATR-FTIR Spectroscopy and Machine Learning

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Linde Methane 2.5 – Gas Cylinder

Linde Methane 2.5 (≥99.5%) gas cylinder for metallurgy, microelectronics, and measurement applications. Reliable fuel and process gas.

Methane 2.5 from Linde is a technical-grade gas with a purity of ≥ 99.5%, supplied in pressurized cylinders for a wide range of industrial and laboratory applications.Due to its properties, methane is an ideal fuel and process gas, particularly for thermal treatments and the creation of controlled atmospheres in metallurgy. It is also used in electronics, microelectronics, and various analytical and physical measurement techniques.Methane 2.5 provides a cost-effective and reliable solution for applications where ultra-high purity is not required but consistent performance is essential.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.5%</li><li>Suitable as fuel and process gas</li><li>Stable composition for industrial use</li><li>Cost-effective solution</li><li>Supplied in pressurized cylinders</li><li>Broad range of applications</li></ul><h4>Technical Specifications</h4><ul><li>Gas: methane (CH₄)</li><li>Purity: ≥ 99.5% (2.5 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 l (200 bar)</li><li>50 l (200bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Metallurgy – controlled atmospheres for thermal processing</li><li>Electronics and microelectronics</li><li>Energy carrier for specialized processes (e.g., explosive surface treatment)</li><li>Standard gas for calorimetric measurements</li><li>Process gas for radioactivity measurements</li></ul>

Linde Oxygen 3.5 – Gas Cylinder

Linde Oxygen 3.5 (≥99.95%) gas cylinder for metal cutting and industrial use. Higher purity improves cutting speed and quality.

Oxygen 3.5 from Linde is a technical-grade gas with a purity of ≥ 99.95%, supplied in pressurized cylinders for industrial and technological applications.Its enhanced purity improves combustion efficiency, increases cutting speed, and enhances cut quality. This makes it ideal for laser, plasma, and oxy-fuel cutting of metals, particularly steels and sheet materials. It is also widely used in electronics, precision engineering, mechanical engineering, and in the production of vehicles, aircraft, and pressure vessels.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.95%</li><li>Supports high-intensity combustion</li><li>Improves cutting speed</li><li>Enhances cut quality</li><li>Suitable for industrial applications</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: oxygen (O₂)</li><li>Purity: ≥ 99.95% (3.5 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>50 l (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Laser cutting of metals</li><li>Plasma cutting</li><li>Oxy-fuel cutting</li><li>Electronics and precision engineering</li><li>Mechanical engineering</li><li>Manufacturing of vehicles, aircraft, and pressure vessels</li></ul>

Linde Oxygen 4.5 – Gas Cylinder

Linde Oxygen 4.5 (≥99.995%) gas cylinder for analytics, chemistry, and semiconductors. High-purity gas for laboratory and industrial applications.

Oxygen 4.5 from Linde is a high-purity gas with a purity of ≥ 99.995%, supplied in pressurized cylinders for demanding laboratory, analytical, and industrial applications.It acts as a strong oxidizing agent in chemical processes and serves as an operational gas for analytical applications. Its high purity ensures minimal contamination and reliable, reproducible results.Oxygen 4.5 is widely used in the chemical industry, semiconductor manufacturing, healthcare, and research, where stable and precise performance is required.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.995%</li><li>Strong oxidizing properties</li><li>Suitable for analytical applications</li><li>Low impurity levels</li><li>Stable and reproducible performance</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: oxygen (O₂)</li><li>Purity: ≥ 99.995% (4.5 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Chemical industry (oxidation processes)</li><li>Semiconductor manufacturing</li><li>Analytical laboratories</li><li>Healthcare</li><li>Research and development</li></ul>

Linde Oxygen 5.0 – Gas Cylinder

Linde Oxygen 5.0 (≥99.999%) gas cylinder for analytics, semiconductors, and research. Ultra-high purity for demanding applications.

Oxygen 5.0 from Linde is an ultra-high purity gas with a purity of ≥ 99.999%, supplied in pressurized cylinders for the most demanding laboratory, analytical, and industrial applications.It acts as a strong oxidizing agent in chemical processes and serves as an operational gas for analytical applications where maximum purity and minimal contamination are critical. Its quality ensures high precision and reproducibility.Oxygen 5.0 is widely used in the chemical industry, semiconductor manufacturing, healthcare, and research and development environments.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.999%</li><li>Ultra-high purity for demanding applications</li><li>Strong oxidizing properties</li><li>Suitable for analytical use</li><li>Minimal contamination levels</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: oxygen (O₂)</li><li>Purity: ≥ 99.999% (5.0 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Chemical industry (oxidation processes)</li><li>Semiconductor manufacturing</li><li>Analytical laboratories</li><li>Healthcare</li><li>Research and development</li></ul>

Linde Oxygen 6.0 – Gas Cylinder

Linde Oxygen 6.0 (≥99.9999%) gas cylinder for ultra-high purity applications in analytics, semiconductors, and research.

Oxygen 6.0 from Linde is an ultra-high purity gas with a purity of ≥ 99.9999%, supplied in pressurized cylinders for the most demanding analytical, semiconductor, and research applications.It functions as a strong oxidizing agent in chemical processes and as a high-purity operational gas for analytical use, where minimizing trace contaminants is essential. Its exceptional purity ensures maximum accuracy, stability, and reproducibility.Oxygen 6.0 is particularly suited for advanced research, microelectronics, and other applications where gas quality is a critical parameter.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.9999%</li><li>Ultra-high purity for critical applications</li><li>Strong oxidizing properties</li><li>Minimal impurity levels</li><li>Suitable for analytical and semiconductor applications</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: oxygen (O₂)</li><li>Purity: ≥ 99.9999% (6.0 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Chemical industry (high-purity oxidation processes)</li><li>Semiconductor manufacturing</li><li>Analytical laboratories</li><li>Healthcare</li><li>Research and development</li></ul>

Linde Helium 4.6 – Gas Cylinder

Linde Helium 4.6 (≥99.996%) gas cylinder for chromatography, leak detection, and industrial use. Reliable carrier and cooling gas.

Helium 4.6 from Linde is a high-purity inert gas with a purity of ≥ 99.996%, supplied in pressurized cylinders for a wide range of industrial and analytical applications.Due to its chemical inertness, low density, and excellent thermal conductivity, helium is ideal for cooling, protective atmospheres, and analytical workflows. It is widely used as a carrier gas in gas chromatography, ensuring stable separations and reproducible results.Helium 4.6 is also applied in leak detection, metallurgy, glass production, laser technologies, and medical gas mixtures.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.996%</li><li>Chemically inert</li><li>Excellent thermal conductivity</li><li>Low density</li><li>Ideal carrier gas for GC</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: helium (He)</li><li>Purity: ≥ 99.996% (4.6 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li><li>50 L (300 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Shielding gas in welding</li><li>Purging in metallurgy and specialty glass production</li><li>Cooling medium in reactors</li><li>Glass fiber manufacturing</li><li>Carrier gas in gas chromatography</li><li>Laser gas mixtures (with CO₂)</li><li>Leak detection</li><li>Medical gas mixtures</li></ul>

Linde Helium ECD – Gas Cylinder

Linde Helium ECD (≥99.999%) gas cylinder for GC-ECD analysis. Ultra-high purity carrier gas for trace-level detection and reliable results.

Helium ECD from Linde is an ultra-high purity inert gas with a purity of ≥ 99.999%, specifically designed for analytical applications in gas chromatography with electron capture detection (GC-ECD).Its extremely low impurity levels make it ideal for trace analysis, where baseline stability and minimal noise are critical. It serves as a carrier and operational gas in GC-ECD systems, commonly used for detecting halogenated compounds, pesticides, and persistent organic pollutants.In addition to analytical use, helium ECD is also suitable for industrial applications such as purging in metallurgy, reactor cooling, glass fiber production, leak testing, and laser gas mixtures.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.999%</li><li>Optimized for GC-ECD applications</li><li>Extremely low impurity levels</li><li>Stable baseline and low noise</li><li>Chemically inert</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: helium (He)</li><li>Purity: ≥ 99.999% (ECD grade)</li><li>Supply form: pressurized gas cylinder<ul><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Carrier gas in gas chromatography (GC-ECD)</li><li>Analytical chemistry – trace-level analysis</li><li>Purging in metallurgy and specialty glass production</li><li>Cooling medium in reactors</li><li>Glass fiber manufacturing</li><li>Laser gas mixtures (with CO₂)</li><li>Leak detection</li><li>Medical gas mixtures</li></ul>

Linde Helium 5.3 – Gas Cylinder

Linde Helium 5.3 (≥99.9993%) gas cylinder for analytics, GC, and electronics. High-purity carrier and purge gas.

Helium 5.3 from Linde is a high-purity inert gas with a purity of ≥ 99.9993%, designed for demanding analytical applications and use in the electronics industry.It serves as an operational, carrier, and purge gas, particularly in analytical chemistry where high stability and low impurity levels are essential. Its physical properties, including low density and excellent thermal conductivity, make it ideal for chromatography, cooling, and protective atmospheres.Helium 5.3 is widely used across industrial and research environments, including metallurgy, glass production, leak testing, laser applications, and medical gas mixtures.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.9993%</li><li>Suitable for analytical applications and GC</li><li>Low impurity levels</li><li>Chemically inert</li><li>Excellent thermal conductivity</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: helium (He)</li><li>Purity: ≥ 99.9993% (5.3 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Carrier gas in gas chromatography</li><li>Analytical laboratories</li><li>Electronics industry</li><li>Purging in metallurgy and specialty glass production</li><li>Cooling medium in reactors</li><li>Glass fiber manufacturing</li><li>Laser gas mixtures (with CO₂)</li><li>Leak detection</li><li>Medical gas mixtures</li></ul>

Linde Helium 5.0 – Gas Cylinder

Linde Helium 5.0 (≥99.999%) gas cylinder for analytics, GC, and industry. High-purity carrier, purge, and measurement gas.

Helium 5.0 from Linde is a high-purity inert gas with a purity of ≥ 99.999%, suitable for a wide range of analytical, industrial, and research applications.It is commonly used as an operational, measurement, and purge gas and is an essential component of gas mixtures for welding and other industrial processes. Due to its chemical inertness, low density, and excellent thermal conductivity, it is ideal for gas chromatography, cooling applications, and protective atmospheres.Helium 5.0 represents a versatile solution for laboratories and industrial environments where high purity, stability, and reliability are required.<h4>Key Features</h4><ul><li>Gas purity ≥ 99.999%</li><li>Suitable for analytical applications and GC</li><li>Chemically inert</li><li>Excellent thermal conductivity</li><li>Versatile use across industries</li><li>Supplied in pressurized cylinders</li></ul><h4>Technical Specifications</h4><ul><li>Gas: helium (He)</li><li>Purity: ≥ 99.999% (5.0 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Carrier gas in gas chromatography</li><li>Analytical laboratories</li><li>Purging in metallurgy and specialty glass production</li><li>Cooling medium in reactors</li><li>Glass fiber manufacturing</li><li>Laser gas mixtures (with CO₂)</li><li>Leak detection</li><li>Medical gas mixtures</li><li>Welding and shielding gas mixtures</li></ul>

Linde Helium 6.0 – Gas Cylinder

Linde Helium 6.0 (≥99.9999%) for GC, analytics, and research. Ultra-high purity carrier, purge, and measurement gas for demanding applications.

Helium 6.0 from Linde is an ultra-high purity inert gas with a purity of ≥ 99.9999%, designed for the most demanding analytical, scientific, and industrial applications.Its extremely low impurity levels make it particularly suitable for highly sensitive analytical techniques such as gas chromatography, where even trace contaminants can impact results. Helium 6.0 ensures excellent stability, reproducibility, and reliability when used as a carrier, purge, or measurement gas.Thanks to its chemical inertness and high thermal conductivity, it is widely used across applications ranging from analytical chemistry to laser technologies and medical gas mixtures.<h4>Key Features</h4><ul><li>Ultra-high purity ≥ 99.9999% (6.0 grade)</li><li>Extremely low impurity levels</li><li>Ideal for high-sensitivity analytical methods (GC)</li><li>Chemically inert</li><li>High thermal conductivity</li><li>Reliable and reproducible performance</li></ul><h4>Technical Specifications</h4><ul><li>Gas: helium (He)</li><li>Purity: ≥ 99.9999% (6.0 grade)</li><li>Supply form: pressurized gas cylinder<ul><li>10 L (200 bar)</li><li>50 L (200 bar)</li></ul></li></ul><h4>Applications</h4><ul><li>Carrier gas in gas chromatography (GC)</li><li>Analytical and research laboratories</li><li>Purging in metallurgy and specialty glass production</li><li>Cooling medium in reactors</li><li>Glass fiber manufacturing</li><li>Laser gas mixtures (e.g., with CO₂)</li><li>Leak detection</li><li>Medical gas mixtures</li></ul>

Products from category Laboratory gases and gas generators - page 3

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