The PD2000 family of high performance molecular characterization detectors, measure absolute values of molecular weight and size. Typical applications are polymers, proteins, antibodies, polysaccharrides and other macromolecules used in the plastics, biotechnology, pharmaceutical and food industries. These laser light scattering detectors are easily added to any HPLC/GPC/SEC system and are ideal research, quality control and process monitoring tools. Available in single, dual and high temperature versions, the PD2000 Series provides cost effective critical path data for any macromolecular characterization application. The PD2040 High Temperature GPC Laser Light Scattering Detector is specifically engineered to provide high performance multi-angle measurements for polymers that are soluble at temperatures ranging from room temperature to 250 degrees C. The PD2040 couples to any commercially available high temperature GPC system (such as those from Polymer Laboratories and Waters Corporation) by direct placement of the light scattering cell inside the system oven compartment and laser outside the oven using a patented coupling design.
Introduction The PD2040 High Temperature GPC Laser Light Scattering Detector is designed to provide absolute molecular weight distributions (Mw, Mn, Mz etc.), radius of gyration (Rg) and branching data for polymers that are soluble only at elevated temperatures. The unit is installed inside the oven compartment of commercially available high temperature GPC systems and operates from room temperature to 250 degrees C. The PD2040 is used in conjunction with Precision Detectors’ new Discovery32™ software. The system provides absolute molecular weight distributions from less than 103 to over 107 daltons and Rg in the 12 nm to 150 nm range.
Key Performance Features for the PD2040
Unique alloy constructed axial platform with high performance 15 degree low angle operates inside high temperature GPC ovens to couple directly to GPC columns and other detectors. This minimizes inter-detector volumes for accurate data and insures sample integrity at GPC system temperature.
Operates from room temperature to 250 degrees C and is compatible with typical GPC solvents for high temperature applications.
10 µL flow cell minimizes sample band-broadening and creates laminar flow within the cell.
Cell design and focused laser beam (to 0.01 µL) eliminates stray light sources and minimizes deleterious GPC system effects (mobile phase and column particulates).
Shielded fiber optic provides high efficiency transfer of detector signals to the electronics module located outside the GPC system.
Discovery32™ software provides an easy to use analyst interface with the system for acquiring, analyzing and reporting GPC data.
The PD2040 High Temperature GPC Laser Light Scattering Detector with Discovery32™ software provides absolute molecular weight distributions and radius of gyration measurements for polymers soluble at temperatures up to 250 degrees C.
Designed for Unparalleled Sensitivity and Stability for Room Temperature to 250 degrees C GPC Environments The PD2040 platform design is optimized for
direct high temperature measurements within
the column oven compartments of modern
GPC systems. The patented axial optical
platform is constructed of specialty alloys
that provide high sensitivity and stability of
the laser light scattering signals under the
thermal stresses present in GPC systems up
to 250 degrees C. These materials
of construction and the ultra-small 10 µL
flow cell provide close coupling of the laser
light scattering platform to the GPC columns
and other detectors (eg. refractive index and
viscometer), providing absolute minimum
inter-detector volumes for accurate data. The
detector incorporates two fixed angle detectors
at 90 degrees and a high-performance
low angle of 15 degrees. The
annular radius of the 15 degree scattering is
collected via a mushroom lens. This unique
optical system provides unparalleled signal-to-noise ratio at low angle to provide accurate
molecular weight data when the polymer
exhibits non-isotropic scattering. The
scattering signals are collected via fiber
optics to the electronics module located outside and transmitted to
the GPC oven. The signal-to-noise ratio
of each detector is optimized by focusing the
laser beam to an optical volume of only
0.01 µL within the 10 µL flow cell. This
minimizes the probability of any “non-sample
scattering”, such as a particle from the
mobile phase or column shedding, from
entering the beam. By collecting data at a rapid
rate (100 points/second) it is now possible
to apply noise rejection algorithms
on
Precision Detectors’ proprietary DSP-based
data-collection board, producing high quality
signals at averaged collection intervals-even
below 1 point per second.
The optical efficiency of the cell is also critical
to the measurement. The PD2040 cell
design, uses separate windows for collection
in a matte black coated cell and unique
“beam dump”. This virtually eliminates stray
light from entering the collection optics thus
minimizing the signal-to-noise ratio. This is
very important as many solvents used in
high temperature applications (eg. 1,2,4
trichlorobenzene) have an intrinsic Rayleigh
scattering intensity almost 30 times that of
water and 8 times that of tetrahydrofuran.
The key issue here is to have the detectors
respond only to signals from the 0.01 µL
optical volume produced by the sample in
solution and not from any stray light source.
Waters Alliance GPC 2000 Series
Polymer Laboratories, Inc. GPC 220
The PD2040 High Temperature Laser Light Scattering Detector is easily configured inside the
column oven of commercially available high temperature GPC systems. Shown here are the Waters Alliance GPC 2000 Series and Polymer Labs GPC 220.
Metallocene Catalyzed Polyolefin Analysis at High Temperature Using PD2040 and Discovery32 Software
Mw vs Elution Time
Figure 1: Laser light scattering and refractive index chromatograms show excellent sensitivity and stability at elevated temperatures.
Figure 2: Discovery32 plot of molecular weight vs. retention time with corresponding calculation of Mw, Mn, polydispersity and Mp (99.65kD, 41.13kD, 2.423 and 92.26kD).
Figure 3: Plot of Radius of gyration (Rg) vs. Mw yields branching data. The exponent of 0.512 indicates the degree of branching. A linear polyolefin would have a value of 0.56.
PD2040 high-temperature light scattering platform – cut-away image showing laser beam and scattering signal paths excluding the extension/inner and heat sink.
Light scattering technology
Light scattering technology has become a popular detection technique in both the lab and plant environment because the answers achieved are absolute and not based on analysis by comparison with calibration curves. PDI's modern designs are popular because they are convenient to use and very stable. The science behind light scattering was first described by Lord Rayleigh at the end of the 19th century but it was not until the 1970s, when polarized lasers became readily available that light scattering technology was applied to practical instruments for laboratory use. At that time, a member of our design team was applying static and dynamic light scattering to instrument designs and was awarded some of the first patents in the field. Today, the analysis of both static and dynamic light scattering signals is well understood. High-performance diode lasers, high-speed digital signal processors (DSP) and other electronic devices are readily available at economical prices. Precision Detectors applies these devices and advanced light scattering technology to the design of the most stable and versatile instruments for lab and plant use.
Rayleigh (static) light scattering
When a polarized, monochromatic laser beam passes through a solvent containing molecules or particles, the excess light scattered at an angle q to the incident beam (ILS) over that scattered by the solvent alone (the base-line) is:
The science behind light scattering was where c is the concentration of the sample in the solvent, Mw is the molecular weight of the sample, (dn/dc) is the change in refractive index with concentration for the sample/solvent pair, P(q) is the ratio of the scattered intensity at angle č to that at angle 0 and K(q) is the optical constant for detection at angle q. A refractometer or other concentration detector following the light scattering detector in the eluant stream detects the concentration signal. Mw is obtained by dividing the light scattering signal by the concentration signal at each elution slice. The radius of gyration (Rg) is obtained from the Debye function using the dissymmetry method. Precision software also calculates Mn , Mz and other averages. The key characteristic of PDI's Rayleigh scattering detectors is their ability to collect the highest-quality signals at angles of 90° and 15° to the incident laser beam. light scattering detection system is its high sensitivity and its unique ability to operate in flow mode with an SEC system calculating R h at each elution slice after chromatographic separation.
Dynamic (quasi-elastic) light scattering
The diffusion coefficient of particles (or molecules) undergoing Brownian movement is related to their hydrodynamic radius (Rh ) as described in the Stokes-Einstein equation:
where k is Boltzman's constant, T is the
temperature in degrees Kelvin, h is the
solvent viscosity and D is the diffusion
coefficient. The diffusion coefficient (D) is
calculated from the reduction time of the
autocorrelation function of the scattered
light. Rh is then calculated.
The key characteristic of PDI's dynamic
light scattering detection system is its high
sensitivity and its unique ability to operate
in flow mode with an SEC system
calculating Rh at each elution slice after
chromatographic separation.