Sustainability Policy

Meritics Sustainability Policy

Meritics Limited are committed to the pursuit of global environmental sustainability.

Concern relating to the avoidance of the depletion of natural resources in order to maintain an ecological balance and sustainability of the planet is integral to our organisation’s management.

We aim to follow and promote good sustainability practices, to reduce the environmental impacts of all our activities and to help our clients and stakeholders do the same.

The policy is based on the following principles:
• The ability to maintain or support our processes over time without depleting natural or physical resources
• To protect the planet, halting climate change and promoting social development without compromising future generations
• To ensure all staff are aware of our Sustainability Policy and are committed to implementing and improving it
• To make clients and suppliers aware of our Sustainability Policy and encourage them to adopt sound sustainable management practices
• To review, annually report and to continually strive to improve our sustainability performance
• To minimise the impact on sustainability on all office and transportation activities
• To comply with all applicable legislation, regulations and codes of practice where relevant

This policy is reviewed yearly

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Comparing FlowCam Results with Light Obscuration

Comparing FlowCam Results with Light Obscuration: A Study by Japan’s National Institute of Health Sciences

In their recent publication, Quantitative Evaluation of Insoluble Particulate Matters in Therapeutic Protein Injections Using Light Obscuration and Flow Imaging Methods, Shibata et. al. compare the ability of Light Obscuration and Flow Imaging to detect and accurately characterize subvisible particles in injectable drugs.

The team at Japan’s National Institute of Health Sciences write the following:

Flow imaging (FI) has emerged as a powerful tool to evaluate insoluble particles derived from protein aggregates as an orthogonal method to light obscuration (LO). However, few reports directly compare the FI and LO method in the size and number of protein particles in commercially available therapeutic protein injections. In this study, we measured the number of insoluble particles in several therapeutic protein injections using both FI and LO, and characterized these particles to compare the analytical performance of the methods. The particle counts measured using FI were much higher than those measured using LO, and the difference depended on the products or features of particles. Some products contained a large number of transparent and elongated particles, which could escape detection using LO. Our results also suggested that the LO method underestimates the size and number of silicone oil droplets in prefilled syringe products compared to the FI method. The count of particles ≥10mm in size in one product measured using FI exceeded the criteria (6000 counts per container) defined in the compendial particulate matter test using the LO method. Thus precaution should be taken when setting the acceptance criteria of specification tests using the FI method.

Read the full publication in the Journal of Pharmaceutical Sciences.

The results of this study corroborate the results produced in our FlowCam lab, comparing particle counts and sizes produced by the two technologies in our new instrument, FlowCam LO.
Our recently produced White Paper, “Measuring Subvisible Particles and Aggregates Using FlowCam LO”, uses FlowCam LO to directly compare the particle size distributions of aqueous samples containing Polystyrene Latex calibration beads, ETFE particles, and IgG aggregates. Download our White Paper to see the results of the study.
FlowCam LO uses two orthogonal techniques in a single instrument by combining our patented flow imaging microscopy technology with an embedded light obscuration particle counter. FlowCam LO provides an even more direct particle count comparison because a single aliquot of sample is analysed by both technologies in one sample run, instead of two samples from the same vial or syringe.

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Privacy Policy

Meritics Ltd Privacy Policy

The Company is committed to the continuous improvement of our systems and processes in order to remain compliant with the General Data Protection Regulation (GDPR)

  • We are committed to telling individuals how and where their information is processed and stored.
  • Upon request we will provide individuals with any information we have on them. Contact us here to make a request.
  • We will only send marketing emails to individuals who have opted-in to the newsletter mailing list.
  • We will never pass individuals details to anyone outside Meritics for them to use for their own marketing purposes.
  • We will ensure that we obtain individuals express consent before we contact them by any method for any purpose.
  • We will make sure our contact with individuals is relevant, based upon the preference information they give us.
  • Individuals can change their contact preferences at any time. Contact us here to make a request.
  • Personal information will be stored safely and will remain secure at all times.
  • We will always delete personal information if requested to do so. Contact us here to make a request.
  • We will always comply with the Data Protection Act 1998 and all other applicable laws and EU Directives.

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Rheological Analysis

Sample Analysis
Rheology

Rheological Analysis

Rheology refers to the analysis of a fluid’s flow or plastic deformation properties relative to shear forces such as rotational torque. It measures the material transportation properties of liquids, solutions, and slurries under distinct mechanical conditions, and enables analysts to accurately plot flow curves and yield points for a range of fluidic materials. This information provides mechanical insights into the coating and flowing properties of numerous commercial and industrial products, from agrochemicals to personal cosmetics.

To assess the rheological properties of a sample, Meritics provides the RM200 PLUS rheometer. This easily-programmable rotational stress rheometer can intuitively measure flow curves of samples with a built-in thermocouple capable of assessing temperatures between -50°C – 300°C.

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Rheometry

Rheology at your fingertips

Thanks to its large storage capacity and its easy programming, the RM200 PLUS allows you to realise all your measurements of flow curves, yield point, thixotropic, fitting without software.

Save your flow curves and calculate your rheological parameters directly without a computer (Plastic viscosity, flow limit, thixotropy, regression model according to Newton, Bingham, Casson and Ostwald). Choose your attachment system tailored to your product constraints.

Contact us for a quote or to discuss your rheological analysis needs.

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Zeta Potential Analysis

Sample Analysis
Zeta Potential

Zeta Potential Analysis by Meritics Specialists

Zeta potential is also known as the electro-kinetic potential of a colloid. It refers to the charge repulsion / attraction of particles dispersed in a solution, and is measured by applying an electrical field to the dispersive medium. Researchers commonly perform zeta potential measurements to ascertain the longevity and mechanical stability of a particulate solution, and to establish particle agglomeration characteristics for pharmaceuticals, food products, and more. The DelsaMax Pro is a rapid zeta potential analyser capable of measuring sample volumes as small as 45 microliters (μL) in under a second. This speed of measurement is crucial for maintaining sample stability and supporting zeta potential characterisation of fast-moving consumer goods, as overlong exposure to electrical fields can cause analytes to degrade – reducing experiment throughput and results accuracy.

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BeNano 180 Zeta Pro Nanoparticle Size and Zeta Potential Analyser Meritics Ltd Bettersize

Dynamic Light Scattering

The BeNano Series is the latest generation of nanoparticle size and zeta potential analysers designed by Bettersize Instruments. Dynamic light scattering (DLS), electrophoretic light scattering (ELS), and static light scattering (SLS) are integrated into the system to provide accurate measurements of particle size, zeta potential, and molecular weight. The BeNano Series is widely applied in academic and manufacturing processes of various fields including but not limited to: chemical engineering, pharmaceuticals, food and beverage, inks and pigments, and life science, etc.

Contact us for a quote or to discuss your zeta potential analysis needs.

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Particle Charge Analysis

Sample Analysis
Particle Charge

Particle Charge Analysis by Meritics Specialists

Powders and granular materials can acquire an electrical charge on the surface of their particles due to contact and movement against handling equipment and containers. Contact and movement of particles within the material itself can also cause charge acquisition. This process is called tribocharging.

It is important to measure particle charge as charge acquisition can lead to problems and unstable behaviour. Charged materials stick to processing equipment and containers, can become airborne more easily, and can flow in different ways than materials with no charge. Many researchers believe that material electrical properties are the most important contributors to powder flow behaviour.

The Mercury Revolution and Volution powder analysers provide particle charge assessments of powdered solid particles during dynamic and stable states when in contact with many different surfaces, including stainless steel, glass, and aluminium.

Volution Powder Analyser

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Volution Powder Analyser

Volution

Flowability is the capacity to move by flow that characterises powders, i.e. loose particulate solids, as well as fluids. If you need an affordable, easy-to-use method to measure the flow properties and bulk characteristics of your powder then you need to be aware of the Volution Powder Flow Tester.

The Volution Powder Flow Tester uses an annular shear cell to measure a powder’s response to consolidating pressure using the yield locus technique. This approach, in conjunction with the instrument’s heavy duty frame and drive system, allows the Volution Powder Flow Tester system to measure powder samples at pressures up to 250kPa (50kg force). This is around 6 times greater than other instruments, which are often more expensive as well.

Cohesion is a measure of particle to particle bonding strength that results from inter-particle forces generated by factors such as electrical charges, moisture and van der Waals forces.

The angle of internal friction is a measure of the force required to cause particles to slide or move or on each other and is influenced by many parameters including particle surface friction, particle shape, hardness, particle size, etc. distribution, etc. As well as the cohesion and angle of internal friction of the material the Volution Powder Flow Tester can also measure wall friction, time consolidation and unconfined yield strength.

The Volution Powder Flow Tester also has built in temperature and relative humidity sensors, which means it will also automatically weigh the sample to provide density and compressibility measurements. Flow functions can be measured by testing the material at different pressures.

Meritics can provide this level of functionality at such low cost because design and engineering all takes place in house, thanks to their experience gained over 20 years in the industry. Due to the geometry of its test cell, the Volution can test granular materials as well as powders, which other shear testers cannot, as the test cells for other instruments are too small. With the ION Charge Module you can even measure powder charge too.

Contact us for a quote or to discuss your particle charge analysis needs.

Revolution

Powder flow property measurements generally fall into two main categories: dynamic analysis and static analysis. Dynamic instruments measure powder flow properties as the test material is moving or is about to move.

Static instruments measure powder that is not moving and typically has been exposed to pressure. For a complete picture of a material’s flow behaviour, both types of testers are required. For solving specific flow problems, usually one type of tester or test is required.

The Revolution Powder Analyser can measure your powder’s ability to flow, consolidate, granulate, cake, pack and fluidise by measuring the power, time and variances in power of your powder in a rotating drum. This data can be used to quantify your powder’s particle behaviour during process applications such as blending, tableting, mixing and transportation. The Revolution is both easy to load and automatic, eliminating the opportunity for human error.

The REVOLUTION Powder Analyser consists of a rotating drum that measures the flow properties of granular and fluidised materials. Several drum sizes are available, from drums requiring 10 cc’s of sample to drums using 500 cc’s.

A stepper motor turns high precision silicone rollers which in return rotates the drum. The operator can set the drum rotation rate (range 0.1 to 200 RPM) and prep time (range 0 to 999 seconds) of the analysis. A digital camera with the assistance of back-light illumination takes digital images of the powder during the rotation process. The images can be accumulated up to a rate of 30 frames per second.

Using patent pending algorithms, the software measures the behaviour of the powder from the images collected due to the drum rotation and how this behaviour changes over time. This data is then used to calculate various parameters representing the powder’s quality and process ability.

Contact us for a quote or to discuss your particle charge analysis needs.

Revolution Powder Analyser

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Powder Flow Analysis

Sample Analysis
Powder Flow

Powder Flow Analysis by Meritics Specialists

The flowability of bulk powdered solids is a crucial parameter for determining an analyte’s proclivity to conglomeration or fluidisation under distinct conditions.

Motion and pressure can cause bulk powders to undergo complex pseudo-phase transitions depending upon the molecular composition and particle geometry of the sample. Particle flow analysis is used to capture imagery of powders under defined mechanical conditions and to characterise the flow characteristics of the material as a proportion of potential energy to flow capacity, and cohesion relating to inter-particle forces.

Meritics supplies a broad range of powder flow analysers for determining the flowability and caking capacities of bulk powders. The Mercury Revolution is an advanced powder flow analyser for assessing the dynamic properties of samples at rotational speeds of up to 200 RPM. The Volution Powder Flow Tester uses an annular shear cell to assess a powder’s physical responses to consolidating pressures of up to 250 kPa.

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Revolution Powder Analyser

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Absolute density of solids and powders is commonly measured through pycnometry, which uses gas displacement to determine the particulate density and purity of compact and granulated solid samples. This method uses a test gas with minute atomic dimensions such as helium to permeate the porous structures of a dry powder or solid sample. The small atomic size of helium enables the test gas to diffuse through extremely narrow pores, providing a volumetric measurement that can be compared to the weight of the dried sample to characterise the real or absolute density of the sample.

Powder flow property measurements generally fall into two main categories: dynamic analysis and static analysis. Dynamic instruments measure powder flow properties as the test material is moving or is about to move.

Static instruments measure powder that is not moving and typically has been exposed to pressure. For a complete picture of a material’s flow behaviour, both types of testers are required. For solving specific flow problems, usually one type of tester or test is required.

Contact us for a quote or to discuss your powder flow analysis needs.

The Revolution Powder Analyser can measure your powder’s ability to flow, consolidate, granulate, cake, pack and fluidise by measuring the power, time and variances in power of your powder in a rotating drum. This data can be used to quantify your powder’s particle behaviour during process applications such as blending, tableting, mixing and transportation. The Revolution is both easy to load and automatic, eliminating the opportunity for human error.

The REVOLUTION Powder Analyser consists of a rotating drum that measures the flow properties of granular and fluidised materials. Several drum sizes are available, from drums requiring 10 cc’s of sample to drums using 500 cc’s.

A stepper motor turns high precision silicone rollers which in return rotates the drum. The operator can set the drum rotation rate (range 0.1 to 200 RPM) and prep time (range 0 to 999 seconds) of the analysis. A digital camera with the assistance of back-light illumination takes digital images of the powder during the rotation process. The images can be accumulated up to a rate of 30 frames per second.

Using patent pending algorithms, the software measures the behaviour of the powder from the images collected due to the drum rotation and how this behaviour changes over time. This data is then used to calculate various parameters representing the powder’s quality and process ability.

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Viscosity Analysis

Sample Analysis
Viscosity

Viscosity Analysis

Viscosity is a measure of a fluid’s resistance to flowing under varying temperature conditions.

It is typically associated with the concept of liquid density or thickness, and usually increases exponentially with decreased temperatures. This property is determined by friction between particles within the liquid or solution and is quantified as a measure of centipoise (cP). Viscosity measurements apply relatively weak thermodynamic forces to a liquid or solution to encourage the material to flow. Temperatures can be increased and torque can be applied to measure the material’s resistance to these conditions, with common applications in the food and beverage, cosmetics, and chemical sectors.

Meritics provides a substantial range of viscosity analysers suitable for a broad range of applications. The RM 100 Portable enables analysts to measure viscosity outside of laboratory conditions with a sustained accuracy of within 1% of the full scale. The First Plus is an ultra-sensitive viscosity analyser with a torque range as low as 0.005 mNm for outstanding precision..

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Viscometers

Unique design removes the problems associated with spring type viscosity measurements. This makes the Lamy range very robust and replacing expensive springs and pointer assembles are a thing of the past!

For ultra-sensitive viscosity measurements, the First Touch features a torque range of 0.005 to 0.8 mNm

With its expanded programming possibilities and increased modularity, the FIRST PLUS will be the ideal tool for your application whether you use it alone or with its software.

Delivery as a single unit or with the spindle sets L1-L4 or R2-R7.

  • Measurement at different speeds
  • Viscosity range up to 240 000 000 mPas
  • 7 “touch screen
  • different measuring spindle sets
  • easy to use
  • wide range of applications
  • stable stand

Contact us for a quote or to discuss your particle analysis needs.

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Density Analysis

Sample Analysis
Density

Density Analysis

Solid materials are regularly characterised relative to their density, which is expressed as the mass of a powder or solid material per unit volume. Density analysis is regularly acquired using a form of gas displacement, which can rapidly determine the real density and purity of solid materials such as ceramics, metals, and polymers.

The Thermo Scientific Pycnomatic is a comprehensive solution for performing density measurements of solid materials. It features a fully-integrated, high-precision temperature control for exceptional results reproducibility. It boasts a real multi-volume capability for utmost accuracy of results with different solid materials, including fine powders and foams.

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Density Analysis BeDensi T Pro Series

BeDensi T Pro 

The BeDensi T Pro series is a reliable tapped density analyser that excels at intuitive operation while complying with the USP, EP, ASTM, and ISO standards. It can measure the bulk density and tapped density with less than 1% repeatability variation to help users to understand the flowability of a wide variety of powder materials.

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Surface Area Analysis

Sample Analysis
Surface Area

Surface Area

Surface area analysis is a common particle measurement methodology that provides data relevant to a material’s adsorption and dissolution properties, as solid particles primarily interact with other media through their surface area. It is possible to determine multiple characteristics of solid materials by assessing the volume of an inert gas that it can adsorb, and the pressure required to push the gas into a porous structure. It is also possible to assess the interaction of gases with the free surfaces of powder particles. Both techniques provide critical insights for manufacturing of dosage form pharmaceuticals.

The Horiba SA-9600 series is suitable for both single- and multi-point surface area analysis with a range of 0.10 – 2,000 square meters per gram.

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SA-9600 BET Flowing Gas Surface Area Analysers, Meritics Ltd Horiba BET

BET Surface Area

Brunauer-Emmett-Teller (BET) surface area analysis is the multi-point measurement of an analyte’s specific surface area (m2/g) through gas adsorption analysis, where an inert gas such as nitrogen is continuously flowed over a solid sample, or the solid sample is suspended in a defined gaseous volume. Small gas molecules adsorb to the solid substrate and its porous structures due to weak van der Waals forces, forming a monolayer of adsorbed gas. This monomolecular layer, and the rate of adsorption, can be used to calculate the specific surface area of a solid sample and its porous geometry, informing studies into the reactivity and bioavailability of pharmaceutical products.

The Horiba SA-9600 can measure BET surface area at a range of 0.10 to > 2,000 m2/g for intervals of just 6 minutes.

Contact us for a quote or to discuss your particle sizing needs.

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Particle Shape Analysis

Sample Analysis
Particle Shape

Particle Shape Analysis

Particle morphology refers to its form, shape, and its physiochemical or biochemical structure. Analysing particle shape and morphology can provide significant insights into the characteristics of a material and its practical applications, as well as its genesis.

There are numerous applications for the observation of particle shape and morphology, including the assessment of drug efficacy and quality control of industrial surface treatments. The FlowCam series of particle counters is equipped to perform particle shape and morphology analysis, with additional parameter considerations for application-specific purposes. Sub-visible proteins of below 10 micrometers (μm) can be quantified using the FlowCam Biologics, while larger particles of between 50 µm – 5000 µm can be morphologically measured using the FlowCam Macro.

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Dynamic Imaging

Today microscopic examination and counting and sizing of small particles is commonplace, Meritics work with Yokogawa Fluid Imaging Technologies (YFIT) and their FlowCam Image Analyser range can size from 300nm to 5mm in range, this takes the tedium involved away and frees up the scientist to analyse data comprehensively.

Electron microscopes probe the size range below the limit of optical microscopy and a scanning technique enables pictures of the surface features of even very delicate surfaces to be made in exquisite detail.

Most recently our scientists have been sizing sugar samples on the FlowCam 8000 to measure the size and to give an image of the particles.

Contact us for a quote or to discuss your image analysis needs.

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Particle Count Analysis

Sample Analysis
Particle Count

Particle Count Analysis

Particle Count Analysis is a broad field of particle analysis, using multiple techniques and methodologies to acquire data about the density and concentration of solid, liquid, or gaseous particles in a sample. High-sensitivity imaging technology, electrical sensing zone (ESZ) techniques, and light obscuration methods are all used to measure the concentration or volume of particles, with proven applications in material characterisation and environmental studies.

At Meritics, we provide Laboratory Analysis using a range of particle counters, including the Multisizer 4e which uses Electrical Sensing Zone analysis; the Spectradyne nCS2 uses resistive pulse sensing to count and size from 2um down to 50nm and the FlowCam range which uses Dynamic Imaging.

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Electrical Sensing Zone

Beckman Coulter Multisizer 4e, with a range of 0.2µm to 1600µm is widely used in many areas: Life Sciences such stem cells, cell biology, and Industrial such as toner, ceramics, sediments etc. as well as Pharmaceutical applications.

The Coulter Principle (also known as ESZ – Electrical Sensing Zone) is hailed as probably the most significant advance in the field of particle technology, and tens of thousands of Coulter Counter instruments are in regular use worldwide.

Most recently our scientists have been running a lot of water samples on the Multisizer 4e to measure contaminants.

Contact us for a quote or to discuss your particle sizing needs.

Resistive Pulse Sensing

The Spectradyne’s nCS2 TM has taken the Coulter Counter method and re-engineered the principle, it is now possible to count and size individual particles down to 50nm.

The Spectradyne nCS2TM instrument provides a unique platform for the rapid quantitative measurement of Nanoparticle size in solution.

The instrument measures individual nanoparticles to produce particle size distributions with quantitative concentration information for particles from 40nm to 2000nm in size. Not relying on optical technology, the Spectradyne system can be used for protein aggregation studies, extracellular vesicle analysis, nanomedicine, virus studies etc.

Disposable microfluidic cartridges eliminate cross contamination and make operation simple and straightforward from just 2-3µl of sample.

Spectradyne’s nCS1 instrument and associated analysis cartridges, are based on Spectradyne’s patented nanoparticle analyzer (NPA) technology. The heart of the instrument is the microfluidic cartridge, which allows the electrical detection of nanoparticles as they pass one by one through a nanoconstriction. Particles larger than the nanoconstriction are removed before reaching it by filters that are built into the cartridge.

No pre-filtering of the sample is required by the user.

Contact us for a quote or to discuss your particle sizing needs.

Spectradyne nCS2 Particle size distribution with absolute concentration

Dynamic Imaging

Today microscopic examination and counting and sizing of small particles is commonplace, Meritics work with Yokogawa Fluid Imaging Technologies (YFIT) and their FlowCam Image Analyser range can size from 300nm to 5mm in range, this takes the tedium involved away and frees up the scientist to analyse data comprehensively.

Electron microscopes probe the size range below the limit of optical microscopy and a scanning technique enables pictures of the surface features of even very delicate surfaces to be made in exquisite detail.

Most recently our scientists have been sizing sugar samples on the FlowCam 5000 to measure the size and to give an image of the particles.

Contact us for a quote or to discuss your particle sizing needs.

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Particle Size Analysis

Sample Analysis
Particle Size

Particle Size Analysis

In all product development, the particle size of products and materials is a critical parameter in their manufacture. Changing the particle size distribution of a material has a massive impact on its characteristics and behaviour either during manufacture, within the final product or on its effects within the environment.

The Meritics Lab offer a range of measurement techniques and particle size analysis testing methods that cover virtually all materials — wet or dry, ranging from >1 nm to 5 mm in size. Our expert scientists can help select the most appropriate test for your material/system from the following:

  • Laser Diffraction
  • Dynamic Light Scattering
  • Electrical Sensing Zone
  • Dynamic Imaging
  • Sieve

Depending on the technique used, we can report:

  • Particle size distribution – weighted to volume, number or surface area
  • Polydispersity

Additionally, Meritics offer a fully validated method development service.

Get in touch for a quote or to find out more about how we can support you ….


Soils analysis particle size distribution laser diffraction particle characterisation granulometry

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Laser Diffraction

Laser diffraction analysis is based on the Fraunhofer diffraction theory. The intensity of light scattered by a particle is directly proportional to the particle size. The angle of the laser beam and particle size have an inversely proportional relationship, where the laser beam angle increases as particle size decreases and vice versa. The particles are placed in a flow cell between the laser and its focal point. The material is analysed using its laser scatter pattern.

The technique of laser diffraction requires the ability to measure the angle of diffraction of the laser light in order to ascribe a size to the particle. For relatively large particles such as 20µm, this is relatively easy as the intensity minima are well defined, see below:

However, once the size gets below 1µm, there is little or any discernible shape to the intensity ‘curve’ making the discernment of any angular variation virtually impossible below approx. 0.4µm.

Some manufacturers take the intensity data down to this size level and then make effectively; an educated guess; at the data below in order to show something down to 0.1µm. Beckman Coulter developed a patented detection system ‘Polarisation Intensity Differential Scattering’ (PIDS) to overcome the limitations of laser diffraction in this region. Particles scatter polarised light by differing amounts. By combining vertically and horizontally polarised light with multi-wavelength measurements, a much more accurate and reliable measurement can be made below 0.4µm.

The approach has been validated by many of the other manufacturers trying to partially copy this by adding additional wavelength measurements.
The most Modern Beckman Coulter LS 13320 XR system can now produce real data down to 10nm using the Patented PIDS system.

Our scientists work with clients across many industries and are experienced in measuring a variety of samples from dry powders such as sugars, soils and sediments to emulsions. If your samples are soluble in water we can measure them in a non-aqueous dispersant, or use a surfactant if it wets poorly. Additionally, we can report means weighted results according to volume, number or surface area.

For submicron particles, the principle of Brownian Motion can be used, as in the Beckman Coulter DelsaMax. Particles suspended in a liquid are in a constant state of random movement or vibration due to the molecular bombardment.

The smaller the particle, the faster it will move. Analysis of the frequency change of scattered laser light pattern is made by auto-correlation spectroscopy, from which average particle size and particle distribution are calculated, the only contestants with this method are the liquids refractive index and viscosity or temperature need to be known. DLS has an overall effective size range of 0.4nmm to 10m.

Our most recent work has been with a lot of university establishments working with crude oil.

Contact us for a quote or to discuss your particle sizing needs.

Beckman Coulter LS 13 320 XR Laser Diffraction Particle Size Analyser 21 CFR Part 11
Bettersizer S3 Plus+BT-803
Viewsizer 3000 Simultaneous Multi-Laser Nanoparticle Tracking Analysis (NTA) Horiba Scientific Meritics Ltd Characterise metal powders whiskey shelf life
Myriade Videodrop Measuring size & concentration of nanoparticles in real time and in a single drop

Spectradyne nCS2 Particle size distribution with absolute concentration

Electrical Sensing Zone

Beckman Coulter Multisizer 4e, with a range of 0.2µm to 1600µm is widely used in many areas: Life Sciences such stem cells, cell biology, and Industrial such as toner, ceramics, sediments etc. as well as Pharmaceutical applications.

The Coulter Principle (also known as ESZ – Electrical Sensing Zone) is hailed as probably the most significant advance in the field of particle technology, and tens of thousands of Coulter Counter instruments are in regular use worldwide.

Most recently our scientists have been running a lot of water samples on the Multisizer 4e to measure contaminants.

Contact us for a quote or to discuss your particle sizing needs.

Spectradyne’s nCS2TM has taken the Coulter Counter method and re-engineered the principle, it is now possible to count and size individual particles down to 50nm.

The Spectradyne nCS2TM instrument provides a unique platform for the rapid quantitative measurement of Nanoparticle size in solution.

The instrument measures individual nanoparticles to produce particle size distributions with quantitative concentration information for particles from 40nm to 2000nm in size. Not relying on optical technology, the Spectradyne system can be used for protein aggregation studies, extracellular vesicle analysis, nanomedicine, virus studies etc.

Disposable microfluidic cartridges eliminate cross contamination and make operation simple and straightforward from just 2-3µl of sample.

Spectradyne’s nCS2 instrument and associated analysis cartridges, are based on Spectradyne’s patented nanoparticle analyser (NPA) technology. The heart of the instrument is the microfluidic cartridge, which allows the electrical detection of nanoparticles as they pass one by one through a nanoconstriction. Particles larger than the nanoconstriction are removed before reaching it by filters that are built into the cartridge.

No pre-filtering of the sample is required by the user.

Contact us for a quote or to discuss your particle sizing needs.

Dynamic Imaging

Today microscopic examination and counting and sizing of small particles is commonplace, Meritics work with Yokogawa Fluid Imaging Technologies (YFIT) and their FlowCam Image Analyser range can size from 300nm to 5mm in range, this takes the tedium involved away and frees up the scientist to analyse data comprehensively.

Electron microscopes probe the size range below the limit of optical microscopy and a scanning technique enables pictures of the surface features of even very delicate surfaces to be made in exquisite detail.

Most recently our scientists have been sizing sugar samples on the FlowCam 8000 to measure the size and to give an image of the particles.

Contact us for a quote or to discuss your particle sizing needs.

FlowCam Macro Flow Imaging Microscopy

Sieves

For the characterisation of bulk goods of different forms and sizes, the knowledge of their particle size distributions is essential. The particle size distribution, i.e. the number of particles of different sizes, is responsible for important physical and chemical properties such as solubility, flowability and surface reaction.

In many industries such as food, pharmaceuticals and chemistry traditional sieve analysis is the standard for production and quality control of powders and granules. Advantages of the sieve analysis include easy handling, low investment costs, precise and reproducible results in a comparably short time and the possibility to separate the particle size fractions. Therefore, this method is an accepted alternative to analysis methods using laser light or image processing.

Contact us for a quote or to discuss your particle sizing needs.

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Chemicals

Industry Information
Chemicals

Why particle characterisation is important in chemical industries

Particle characterisation is a crucial process in the automotive industry that involves the analysis and understanding of the properties and behaviour of particles present in various automotive components. These particles can be found in engine lubricants, brake pads, fuel, and many other materials used in cars.

By characterising these particles, engineers can gain valuable insights into their size, shape, composition, and distribution. This information helps them in designing and developing more efficient and reliable automotive parts. For example, understanding the particle size distribution in engine lubricants can help engineers create lubricants that provide better protection and reduce friction, leading to improved engine performance and fuel efficiency.
Particle characterisation also plays a vital role in ensuring the safety of automotive components. By analysing the particles in brake pads, engineers can determine their wear rate and composition, helping them develop brake pads that offer optimal stopping power and durability.
Overall, particle characterisation in the automotive industry is a crucial science that enables engineers to create better-performing and safer automotive components, resulting in a smoother driving experience for all.

Case study

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Instruments to support chemical manufacturing

Applications to support chemical manufacturing

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Breakthrough Curves

Technology
Breakthrough Curves

Breakthrough curves: dynamic sorption of gas- and vapor mixtures

Investigation experiments of practically relevant separation processes by standard gas sorption instruments for pore size analysis are limited.

BioLector Microbioreactor

Regarding the assignment of tasks such as

  • investigation of the adsorption of CO2 from dry and wet air
  • adsorption of methane of biogas
  • differentiation of practically relevant sorption behaviour of adsorbents like gas or vapor mixtures.
  • BET- or pore size distribution cannot predict or model separation processes.

The dynamic flow method is applied for practical investigation such as

  • dynamic gas flow adsorption and desorption
  • determination and evaluation of breakthrough curves
  • investigation of sorption kinetics
  • investigation of co-adsorption and replacement effects
  • determination of sorption selectivities
  • determination of sorption equilibria of gas mixtures
  • transfer of technical sorption processes to lab-scale
  • investigation of thermal balance of dynamic adsorption processes

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Measuring method

The figure above shows a breakthrough curve of CO2 at activated carbon measured with the mixSorb L. The vertical, red line marks the start of the breakthrough measurement. From this point a gas mixture of 5 Vol.-% CO2 in Helium flows through the adsorbent at a pressure of 5 bar at 40 °C with a flow of 1 L min-1. The black line represents the concentration of CO2 at the end of the adsorber column. One can observe that after 15 minutes traces of CO2 are detected. Before that time CO2 is completely withheld by adsorption on the activated carbon followed by a steep increase of the CO2 concentration, which is called mass transfer zone. From the shape of the breakthrough curve in this zone different parameters concerning sorption kinetics or concentration distribution can easily be determined. After approximately 30 minutes the activated carbon reaches the maximum sorption capacity under this experimental conditions. Consequently the CO2 concentration at the end of the column approaches the initial CO2 concentration.

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The releasing heat of sorption results in a temperature increase of the adsorber bed. To follow this process the mixSorb L is equipped with four temperature sensors along the adsorber. Their position is sketched at the right side of the figure. The four sensors respond in accordance to the direction of the gas flow starting with T1 and ends with T4. The measured temperature curves (orange, grey, yellow and blue) are also depicted. They give information of the released heat, the speed of energy exchange processes and the dispersion of the concentration profile in the adsorber column.

The following figure illustrates how to determine the technical usable sorption capacity from a breakthrough curve under certain experimental conditions. The BET surface area or the micropore volume, which are exactly known by standard gas sorption methods, are not accessible completely in technical flow processes for certain kind of purification or separation processes. As an example: The separation of CO2 from N2 (40 °C, 2 L min-1, 5 bar, initial gas composition: 5% CO2 in N2) occurs with the breakthrough of CO2 when the sorption capacity reaches 75% of the maximum sorption capacity. The dynamic sorption analyzer mixSorb L can help to predict technical relevant sorption processes in an easy a quick way.

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Chemisorption

Technology
Chemisorption

Chemisorption

The chemisorption analysis is specially used to characterize catalysts. The most crucial point is to determine the chemically active part of the surface area. To determine the active surface area a measuring gas is used, which is able to strongly chemisorb at the active sites. Hydrogen gas is often used for the analysis, which creates a chemisorption bond to noble metals (e.g. platinum-alumina catalysts).

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1. Static-volumetric method

A certain amount of gas is dosed onto the active material in vacuum. The determination of the amount of adsorbed gas is carried out by pressure measurement in a system with known volume. Typically two isotherms are measured during the chemisorption experiment: The first isotherm reflects the sum of physisorption and chemisorption. After that the sample is evacuated to desorb loosely bonded gas molecules (physisorbed measuring gas) from the surface. Repeating the isotherm then only shows the physisorption again due to the blockage of the active sites from the first isotherm. Subtracting the second from the first isotherm only reveals the pure chemisorption. From this isotherm the amount of active sites can be calculated.

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2. Dynamic method

2.1. Isotherm (Pulse chemisorption)

An inert gas continuously flows over a solid. A thermal conductivity detector analyses the measuring signal (base line). After that pulses of the measuring gas are added successively into the flow of the inert gas and after each pulse the instrument waits until the signal reaches the base line again. Initially the active material chemisorbs the measuring gas. After a while the actives sites are getting saturated. The measurement is being continued until the thermal conductivity detector shows constant peaks and no measuring gas is chemisorbed any more. This method is called pulse- or titration method.

Chemisorption experiments are often carried out temperature-controlled, please read more at measuring method „temperature-programmed reactions“.

2.2. Temperature-programmed reactions

Non-isothermal measurements are carried out usually through linear heating of a sample and continuous recording the changes of the gas composition. Temperature-controlled reactions can involve desorption (TPD), reduction (TPR), oxidation (TPO) and other relevant reactions for the characterization of catalysts.

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Before performing temperature-controlled reactions to characterize catalysts the sample is prepared in-situ. Therefore so-called macros are defined, so that the procedure of the sample preparation is done fully automatically. The further approach is then task-oriented: A TPD experiment starts with the adsorption of active gas on a sample (e.g. by pulse chemisorption) followed by the characterization of the temperature-dependent desorption process. TPR reactions are done using a reducing gas, usually H2, TPO experiments are performed with an oxidizing gas, typically O2.

The experiments are carried out in a gas flow and changes in the gas composition are recorded by the thermal conductivity detector. Before performing an experiment, it has to be considered that not only the gas composition has to change during the reaction, also the thermal conductivity has to change due to ad- and desorbing molecules. In principle gases and vapors can be divided up into two main groups regarding their thermal conductivities:

1. H2, He
2. CO, CO2, Ar, NH3, H2O, Pyridin, N2O etc.

By this classification, the experiments can be easily derived. During a chemisorption reaction a gas/vapor from both group has to be present. Examples:

  • 1. TPR with hydrogen (group 1) needs a carrier gas from group 2, e.g. Argon.
  • 2. TPD of NH3 (group 2) requires a carrier gas from group 1, typically Helium.
  • 3. TPO with Oxygen (group 2) needs a carrier gas from group 1, e.g. Helium.

The advantages of temperature-controlled reactions are not only to determine the active sites of catalysts but also determining on the different strengths of chemically active sites due to the temperature dependence.

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Vapour Sorption

Technology
Vapour Sorption

Vapor sorption: DVS (dynamic) and SVS (static-volumetric)

The determination of water uptake and -release is highly important for a lot of products for their application, their behavior in processes or storage issues. Water uptake can be determined as a function of relative humidity. In other projects water or other vapors are used as sensors to investigate the interaction between molecules with different polarities and surfaces and compare these interactions with other molecules. Due to practical reasons the properties of porous materials under humid conditions have to be well known. Different prospects are possible to investigate the sorption behavior of gas-vapor or vapor-vapor mixtures.

Measuring methods

1. Dynamic vapor sorption – DVS

Water vapor sorption follows the same physical rules and principles as gas sorption. The difference to gas sorption is that condensation of vapors must not influence the results of the measurement. Because of this reason, the water uptake is often measured gravimetrically in a dynamic, humid gas flow (DVS – Dynamic Vapor Sorption) – these experiments can be carried out for many materials, such as pharmaceutical products, food, packing materials, building materials etc.

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2. Static-volumetric vapor sorption

Water vapor sorption can also be measured static-volumetrically in a measuring system with calibrated volume by measuring the equilibrium pressure. Corresponding analyzers exhibits a heated volume system, so that condensation in the manifold, valves or lines is avoided. The liquid is stored in a glass-vessel, which is connected to the manifold with a valve/line-system. First the glass-vessel is evacuated to remove the air then the desired vapor phase is build up above the liquid phase. Dosing of this vapor into the measuring cell removes vapor from the manifold, more liquid from the glass-vessel is evaporated until the equilibrium state between liquid and gas phase is reached again.
Determination of the water sorption isotherm (ad- and desorption) are carried out fully automatically and different possibilities are offered for the analysis of isotherms: Determination of surface areas, pore volumes or heats of adsorption.

3. Mixture adsorption of vapors

Another possibility is the determination of the sorption behavior of vapors in gas-vapor or vapor-vapor mixtures with the mixSorb S and mixSorb L series. Practical questions can be directly studied, e.g. investigation of the sorption behavior of humid adsorbents in a dry gas flow or the sorption behavior of adsorbents under a humid gas-vapor flow. There is a huge difference between these two cases and both experiments can easily be prepared. Such investigations can be done flexibly with the mixSorb series including the coupling to external analytical devices to determine e.g. trace elements.

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Adsorption of Mixed Gases

Technology
Adsorption of Mixed Gases

Adsorption of mixtures: Dynamic sorption of gas and vapor mixtures

Challenges such as the adsorption of CO2 from dry and moist air, the adsorption of methane from biogas or the differentiation of the relevant physisorption behavior of adsorbents in gas and vapor mixtures are different from classical methods for texture determination. The main reason here is the fact, that a sorption of mixtures is occurring and the mixture needs to be separated accordingly in order to discover, which component is adsorbed at which magnitude.

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Especially the selectivity plays a crucial role in the adsorption of mixtures, since the task requires the stronger adsorption of one component within the mixture in comparison to other residual components. In order to predict or model technical processes and extract data with practical relevance, the following investigations become more and more important:

  • dynamic adsorption and desorption from a gas flow
  • determination and evaluation of breakthrough curves
  • investigation of sorption kinetics
  • investigation of co-adsorption and displacement effects
  • determination of sorption selectivity
  • determination of sorption equilibria in gas and vapor mixtures
  • scaling of technical sorption processes
  • investigation of heat balance in dynamic adsorption processes

Analytical method

In order to minutely project technical adsorption processes, a representative selection of sample as well as an authentic representation of the flow field is required within the reactor bed.

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The standard column of the mixSorb L with a volume of roughly 100ml and an internal diameter of 3cm has been modelled precisely towards these characteristics. The robust construction from stainless steel allows for experiments at temperatures up to 450°C and pressures of up to 10bar. Four Pt-100 thermo-couples positioned equidistantly along the reactors columns central vertical axis and allows for high resolution recording of temperature profiles within the reactor bed. Up to four internal mass-flow controllers allow for the arbitrary composition as well as streaming speed of gas mixtures. The detection and composition of gases and mixtures is carried out by an internal thermal conductivity detector or an additional mass spectrometer. Reversion of the flow direction within the column allows for in-detail studies of desorption processes in technical adsorbents. This allows for the investigation of regenerative capabilities as well as cyclic durability of technical adsorbents while at the same time allowing for the simulation and investigation of complex pressure swing adsorption processes (PSA).

Example

The following scheme exemplifies the possibilities of the mixSorb L for investigating the characteristics of practical relevance within the separation of air on a carbon-based molecular sieve. The influence of temperature on the cycling time of the adsorber as well as the breakthrough speed of oxygen was investigated. These methods require the mixSorb-software mixSorb Manager, which handles dosing, measurement and data recording and reduction fully automated.

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Furthermore, the mixSorb L comes with the simulation software 3P-Sim, which is an extraordinary tool for comparing experimental and theoretical data and calculating the experimental effort required for certain tasks by calculating gas mixture data from pure gas isotherms. The figure below showcases how diffusion parameters are merged into the linear driving force (LDF-) factor and below that, how fitting of the mass transfer coefficient kLDF describes experimental curves (both breakthrough and temperature curve) in the software simulation.

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Gas Adsorption

Technology
Gas Sorption

Gas adsorption: pore volume and pore size distribution

Gas adsorption for surface and pore analysis offers solutions for pore characterization between 0.3 nm and approx. 500 nm. The determination of BET surface areas and further methods to characterize pores are described on this website as separate methods. In principle the smallest pores are filled first with gas molecules. With increasing pressure successive pore filling of the larger pores takes place. Based on different evaluation models calculations are done to determine pore volumes or pore size distributions. The advantage of gas sorption lies in performing pore analytics of very small pores (micro- and mesopores).

Measuring method

1. Adsorption isotherm

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The figure illustrates the classification of isotherm and hysteresis types according to the surface and pore structure of non-porous, micro-, meso- and macroporous materials. Besides BET surface area calculations (see corresponding method on this website) isotherms are used to determine pore volumes (micropore- and total pore volume) as well as pore size distributions. Traditional models are e.g. the BJH method for mesopore analysis, the Gurvich rule for total pore volume calculations or Dubinin equations for micropore analysis. To improve these models different groups around the world develop new calculation models. State-of-the-art models are the so-called DFT (density functional theory) models and Monte-Carlo simulations.
In contrast to mercury porosimetry gas adsorption offers different advantages such as mercury-free and easy handling with measuring cells. The measuring range already starts in the micropore range (approx. 0.3 nm) which is not accessible by mercury porosimetry.

Example

The following figure shows an isotherm of a MCM-41 material measured with Nitrogen at 77 K. The applied evaluation models depends on the type of isotherm and therefore on the kind and ratio of pores. For small mesopores the classical BJH- and modern NLDFT methods were applied. These results show that both methods differ and the real pore size of approx. 4.1 nm could not be calculated exactly by the BJH method.
Due to the large number of calculation methods for adsorption isotherms 3P Instruments offers advanced training in terms of surface- and pore characterization analysis to exchange experiences.
During this training various topics are discussed such as sample preparation, measuring and interpretation of different kind of solids by means of concrete examples.

Adsorotion

2. Gas adsorption at different temperatures

Pore size analysis by gas sorption is usually done in a relative pressure range between 0 and 1 by measuring the isotherm of gas at its boiling point. Due to the costs and availability of liquid Nitrogen, normally Nitrogen isotherms are measured at 77 K. In principle each gas can be used at different temperatures to investigate the sorption behaviour or to discuss the analysis of the pore structure data also in terms of practical separation processes. Following gas sorption methods have been proved:

  • Argon at 87 K for micropore determination according to the IUPAC classifications
  • Krypton at 77 K to determine small BET surface areas.
  • Krypton at 87 K to analyse small mesopores in thin, porous layers
  • CO2 at 273 K to investigate small micropores < 1.5 nm
  • H2, CH4, CO2 etc. at different temperatures to investigate gas storage applications
    various adsorptives at different measuring temperatures to compare adsorption processes or the validation of substance-specific parameters and interpretation models for pore analysis
  • Isotherms of an adsorptive at different temperatures to calculate adsorption enthalpies (isosteric heats of adsorption)
  • Chemisorption: H2, CO, NH3, pyridine etc. to characterize active surfaces of catalysts
  • practical relevant investigation of gas- and vapor mixtures by dynamic sorption methods

Example

Isotherms of Nitrogen at 77 K, CO2 at 273 K and H2 at 77 K were measured on a zeolite 4A. In comparison to hydrogen at 77 K or CO2 at higher temperature, Nitrogen shows almost no adsorption at 77 K. This example shows that Nitrogen measurements at 77 K are not the appropriate method to analyze micropores smaller than 0.5 nm. Other adsorptives than Nitrogen and temperatures have to be used. Our LabSPA (Lab for Scientific Particle Analysis) performs test and contract analyses of different kind of gases at various ranges of temperature and pressure.

Adsorotion

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ezSPR

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ezSPR

Benchtop SPR

  • Core technology
  • Flexible design
  • Rapid data processing

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Beckman Coulter LS 13 320 XR Laser Diffraction Particle Size Analyser 21 CFR Part 11

Core Technology

Basic thin film SPR found in most benchtop devices capable of detection in complex media such as serum, plasma, cell lysates, or wastewater.

Flexible Design

Adaptable from injection to sensor. Comes with two injection models with multiple options to meet your research needs

Rapid Data Processing

Intuitive software providing key data for biosensing and protein interaction characterization in real time.

  • Key Features

    • Thin film-based Kretschmann configuration SPR
    • Switchable manual or sample loop injection mode
    • Two sensing channels
    • Two independent pump with sample injection loops
    • Each loop injection volume 100 micro L
    • Sensitivity: 2750 nm/RIU
    • Resolution : 1 micro RIU
    • Dynamic range: 1.33 to 1.39 refractive index unit
    • Coefficient of variation on signal: < 0.6%
    • Polychromatic light source
    • ezControl™ graphic user interface
    • Output data compatible with TraceDrawer™
  • Applications

    Gene Regulation

    Environmental Waters

    Protein-small molecule interation

    Immunosensing

    Antibody QC

    Protein-Protein

    Protein

    Vaccine

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BET Surface Area

Technology
BET Surface Area

Gas adsorption: Determination of the specific surface area (BET surface area)

The determination of specific surface areas represents a major task regarding the characterization of porous and finely-dispersed solids. Gas adsorption is the appropriate method to solve this task. If a gas gets in contact with a solid material a part of the dosed gas molecules is being adsorbed onto the surface of this material. The adsorbed amount of gas depends on the gas pressure, the temperature, the kind of gas and the size of the surface area. After choosing the measuring gas and temperature, the specific surface area of a solid material can be reliably and comparably calculated from the adsorption isotherm. Due to practical reasons the adsorption of Nitrogen at a temperature of 77 K (liquid Nitrogen) has been established as the method for the determination of specific surface areas.

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Measuring method

Speaking about the BET method, actually means the analysis of isotherm data by a method developed by Brunauer, Emmett and Teller. By means of the BET equation the amount of adsorbed gas, which build up one monolayer on the surface, can be calculated from the measured isotherm. The amount of molecules in this monolayer multiplied by the required space of one molecule gives the BET surface area. Besides the adsorption of Nitrogen at 77 K, Krypton adsorption at 77 K is recommended for the determination of very small surface areas.

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Closed cell content

Technology
Closed Cell Content

Closed cell content in foams

The determination of closed and open cell content in foams is based on the determination of the samples volume by means of gas pycnometry, which is an analytical method for density and volume analysis described separately on this homepage. When investigating foams, the most common challenge is to determine the amount of vesicular polymer cells completely closed, as these cells determine the insulation capacities of rigid foams commonly used in the thermal insulation of housing.

Measuring principle

The measurement is carried out as stated per DIN ISO 4590 „Determination of the volume fraction of open and closed cells in rigid foams“. Initially, a geometrically exact sample body will be cut (cube, cuboid or cylinder) and its exact dimension will be determined by means of a micrometer in order to calculate the geometric volume. Afterwards, the sample body will be analyzed in the pycnometer at a low pressure of roughly 0.25 bar. The analytical gas employed here is nitrogen, as helium will penetrate into the walls of the closed cells in the foam. This first measurement includes the volume of the sample body yielding the closed volume, into which the analysis gas cannot penetrate and from which the amount of closed cells will be derived. The so-called uncorrected method terminates here, the quotient from closed volume to geometric volume multiplied by 100% determines the percentage of closed cell content in the sample.

In the so-called corrected method relates to the fact that by cutting through the sample cells previously closed will be opened. This can be corrected by an additional measurement. For this, the sample body will be cut into smaller parts and all parts obtained after cutting will be measured in the pycnometer again. The amount and position of cuts as well as the equation for results depend on the geometry of the original sample body and can either be determined by DIN ISO 4590 or by measuring.

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Gas Pycnometry

Technology
Gas Pycnometry

Determination of density by means of gas pycnometry

In general terms density is defined as the quotient from mass by volume. Mass can be determined with ease by a scale. The determination of volume is more challenging, usually due to samples having irregular shapes or being powders of varying degree. Additionally, it needs to be noted that volume, and thus density, may be defined differently if pores are included (raw density) or excluded (true / absolute density) into the solid samples volume. The density is based on the solid samples volume excluding the pore volume of porous solids.

Gas Pycnometry

With a pycnometer (Greek, „gauged vessel”) the amount of a certain medium (liquid or Helium or other analytical gases) displaced by a solid can be determined. Examples for the use of density determinations for finely ground or bulky solids include, but are not limited to, for example the differentiation between solids, quality insurance, determination of open and closed pore volume in foams and determination of so-called vacuolar volume in the quality control of milk powders. These fields illustrate the versatility of gas pycnometry and exceed the limits of liquid pycnometry. The main advantages of the gas pycnometry are:

  • fast
  • precise
  • requires no organic liquids
  • low user expense
  • automatisation

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Laser Diffraction

Technology
Laser Diffraction

Introduction

The particle size distribution is a crucial parameter in many applications that involve powders or dispersions. These include construction materials like cement and sand, pharmaceuticals, ceramics, colored pigments, fertilizers, emulsions, and more. As the range of applications expands, so do the requirements for measuring methods in terms of size range, measurement time, and reproducibility.

Measuring particles close to the range limits and simultaneously detecting particle sizes of both small (nanometer range) and large particles (lower millimeter range) for polymodally or broadly distributed samples is particularly challenging. However, modern laser diffraction particle size analyzers such as the Bettersizer S3 Plus overcome these challenges through innovative optical system design that detects backscattered light of very small particles and captures large particles with an integrated high-speed CCD camera or a combination of laser diffraction method and image analysis method.

Measuring Method

Laser diffraction method of particle sizing involves the interaction of laser (monochromatic and coherent light) with particles that need to be measured in terms of their size. The diffraction of light waves by the particles follows a distinct pattern depending on their size: larger particles scatter more light in the forward direction. For particles smaller than 100 nm, the scattering intensity is almost the same in all directions.

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The scattering intensity is determined by stationary detectors depending on the angle. State-of-the-art laser diffraction systems such as the Bettersizer S3 Plus laser diffraction particle size analyzer guarantee the determination of scattering intensities in a continuous angular range of 0.02 – 165°, i. e. in the forward, side, and backward direction. This is achieved by means of the unique Dual Lens and Oblique Incidence (DLOI) optical system: Fourier lenses (collective lens) are positioned between the laser and particles as well as between particles and detectors. The particles will interact with the light within a parallel laser beam. This offers the advantage that the scattered light can also be detected at very large angles (in the backward scattering direction) and thus even very small particles can be detected and measured precisely. Thanks to DLOI technology, the problems of conventional measurement setups can also be avoided. Therefore, neither the suitable lenses for the corresponding particle size measurement range have to be selected prior to the measurement (in comparison to the Fourier optics), nor do measurement inaccuracies result from different particle-to-detector distances if not all particles lie in one plane (in comparison to the inverse Fourier optics).

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To calculate the particle size distribution from the measured scattering spectra, the theory of either FRAUNHOFER or MIE is applied. The FRAUNHOFER theory is based on the hypothesis of opaque and spherical particles: the scattered pattern corresponds to a thin opaque two-dimensional plate – diffraction only occurs at the edges. Therefore no additional optical input constants of the material are necessary for this calculation. In contrast, the MIE theory uses the hypothesis of virtually translucent and spherical particles, meaning that light permeates the matter and is scattered elastically at the atoms of the particle. The knowledge of the complex refractive index of the particles and the liquid as well is necessary. This theory is applicable to particles of all sizes.

The following figure shows an example of a volume-weighted particle size distribution of a calcium carbonate powder – measured with a Bettersizer S3 Plus. The cumulative throughput curve (blue line) and the resulting histogram (black bar) can be seen.

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Image Analysis

Technology
Image Analysis

What is image analysis?

The term “image analysis” is describing the mechanism: the image analyzer will capture an image of a 3-D particle first, then do the analysis based on the 2-D particle projection image. Depending on the movement state of particles during the measurement, the image analysis method is divided into 2 kinds: one is the dynamic image analysis method (DIA), and another is the static image analysis method (SIA).

Why Image Analysis?

Today, particle size alone may not be sufficient to get qualified products out the door. Many industries are turning to particle size and shape analysis. This is where the image analysis method comes in. The necessity for size and shape analysis of every single particle, combined with ever-increasing PC processing power, ensures that automated imaging methods are becoming increasingly more relevant to a market which is taking advantages of non-spherical particles.

Automated imaging methods for the determination of the particle size distribution of a material offers a fundamental advantage over alternative methods such as static light scattering, sedimentation or sieving: Each particle is photographed and thus analyzed individually! In addition, the individual photography of the particles gives the opportunity to make statistical calculations of not only the particle size but also the particle shape, this results in several important advantages for the determination of the particle size (shape) distribution:

  • Realistic proportional values also at the edges of the size distribution, i. e. detection of oversized particles or fine particles
  • More meaningful size and shape parameters of each single particle, instead of diameter of ideal spheres. e. g. geodetic length or elongation for fibers.
  • For more information, please check the particle size and shape parameter guidebook
  • Flexible changeovers between distribution types (volume / area / number) depending on the particular task
  • Visual assessment of the dispersing state of a sample (dispersing quality, presence of agglomerates)
  • Further differentiation of materials. For example, in addition to the particle size distribution, the roughness of the particle surface plays an important role for the success of shaping or polishing.

How to Image Analysis?

The determination of the particle size and shape by image analysis method includes 4 basic steps:

1. Image taking

The image taking process is the base of the image analysis method. Special digital cameras are ultilized to ensure a clear vision contains sharp images of particles. If necessary, the camera can be in combination to a microscope.

2. Image processing and particles detection

Appropriate software processes captured pictures: signal noise, isolated pixels and edging particles are eliminated, brightness is adjusted to strengthen the contrast between the particle and the background, etc.

Particles are then separated from the background. Depending on the application, special requirements will be employed to filter out part of particles, such as agglomerates, bubbles, or reflecting metal powders.

3. Particle size and shape calculation

Size and shape parameters of every single particle will be calculated with the software.

4. Statistical calculations and classification

The particles are arranged in classes (e.g. size equivalent classes) on the basis of their attributed features (size and shape parameters).

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Using PIDS Technology

Particle Size Analysis
Capabilities

The LS 13 320 XR particle size analyser uses advanced laser diffraction and PIDS technology for the sizing of non-spherical, sub-micron particles.

Beckman Coulter LS 13 320 XR Laser Diffraction Particle Size Analyser 21 CFR Part 11

Initially, particle sizing by laser diffraction was limited to the use of the Fraunhofer diffraction theory. Laser diffraction offers a number of advantages – laser diffraction analyzsers go beyond simple diffraction effects. General approaches are now based on the Mie theory and the measurement of scattering intensity over a wide scattering angular range is employed.

Using PIDS Technology

Pioneered by Beckman Coulter, most laser diffraction manufacturers use the above two approaches, i.e., wide angular detecting range and short wavelength, to size small particles. However, sizing even smaller particles (tens of nanometers in diameter), cannot be achieved using only these two approaches. Any further increase in scattering angle will not yield any significant improvement due to the everslower angular variation. Figure 2 is a 3-D display that illustrates the very slow angular variation for small particles. For particles smaller than 200 nm, even by taking advantage of the above two approaches, it is still difficult to obtain an accurate size.

Then, two different routes were developed among instrument manufacturers. One is to extrapolate from the measured lower limit to an even lower limit, sometimes even beyond the theoretical lower sizing limit, e.g., 10 nm. Certainly this brings uncertainty or even completely wrong information in the extrapolated region. The other approach is to use the polarization effects of the scattered light.

Vertically polarized scattered light has different scattering patterns and fine structures from that of horizontally polarized light for small particles. The main characteristic of the horizontal scattering intensity (Ih) for small particles is that there is a minimum around 90 degrees. This minimum shifts to larger angles for larger particles. Thus, although both vertical scattering intensity (Iv) and (Ih) have only small contrast in the case of small particles, the difference between them can reveal a more distinguished fine structure, thereby making the sizing of small particles possible. Combining polarization effects with wavelength dependence at large angles, we can extend the lower sizing limit to as low as 10 nm, almost reaching the theoretical limit. This combined approach is known as the Polarization Intensity Differential Scattering (PIDS) technique patented by Beckman Coulter.

The origin of polarization effects can be understood in the following way. When a very tiny particle, much smaller than the light wavelength, is located in a light beam, the oscillating electric field of the light induces an oscillating dipole moment in the particle; i.e., the electrons in the atoms comprising the particle move back and forth relative to the stationary particle. The induced motion of the electrons will be in the direction of oscillation of the electric field, and therefore perpendicular to the direction of propagation of the light beam. As a result of the transverse nature of light, the oscillating dipole radiates light in all directions except in the direction of oscillation; if the detector is facing the direction of oscillation it will receive no scattering from single dipoles. When the light beam is polarized in either the v direction or the h direction, the scattering intensity Iv and Ih for a given angle will be different. The difference between Iv and Ih (Iv – Ih) is termed the PIDS signal. As particle size increases the intra-particle interference makes the particle’s behaviour deviate from that of a simple dipole and the scattering pattern will become more complex. For small particles the PIDS signal is roughly a quadratic curve centered at 90 degrees. For larger particles the pattern shifts to smaller angles and secondary peaks appear due to the scattering factor. Since the PIDS signal is dependent on particle size relative to light wavelength, valuable information about a particle size distribution can be obtained by measuring the PIDS signal at several wavelengths.

Figure 4 displays the shift in the peak value and the change in contrast for particles of various diameters are clearly shown. In addition, because the PIDS signal varies at different wavelengths (it becomes flatter at longer light wavelengths), measurement of the PIDS signals at several wavelengths will provide additional scattering information that can be used to further refine the size retrieval process.

From Figure 4, the angular patterns for 100 nm and even for 50 nm particles are recognizable, in addition to the shift in the axis of symmetry. It has been verified through both theoretical simulation and real experimentation that accurate sizing of particles smaller than approximately 200 nm by scattering intensity without the use of the PIDS technique is practically difficult and probably unrealistic. The combination of the three approaches (wider angular range, wavelength variation, and polarization effects) improves the accurate characterization of submicron particles using light scattering.

Figure 5 is a typical trimodal distribution retrieved in a laser diffraction experiment using the PIDS technique at multiple wavelengths (λo = 475, 613, 750 and 900 nm) and over a scattering angular range with angles up to 144 degrees, with (solid line) and without (dashed line) using the polarization effect. The dotted lines represent the nominal diameter values of the latexes in the mixture as reported by the PSL vendor. Without the PIDS technique the smallest component is missed, even when using the information gathered at large scattering angles and short wavelengths. Figure 6 is an SEM image of the sample in Figure 5 in which three different sizes of particles can be seen.

In summary, only using all three approaches, i.e., wide angular range, short wavelength and polarization effect, can particle size as small as 10 nm can be correctly measured, not extrapolated. There is no mixing of technologies. All signals are from the same scattering phenomenon and treated integrally in a single data retrieval process just like in an ordinary laser diffraction measurement.

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