The information in this document is subject to change without notice and
should not be construed as a commitment by Waters Corporation. Waters
Corporation assumes no responsibility for any errors that may appear in this
document. This document is believed to be complete and accurate at the time
of publication. In no event shall Waters Corporation be liable for incidental or
consequential damages in connection with, or arising from, its use.
Trademarks
Waters is a registered trademark of Waters Corporation. Empower, e-SAT/I N,
and MassLynx are trademarks of Waters Corporation.
Other trademarks or registered trademarks are the sole property of their
respective owners.
Customer comments
Waters’ Technical Communications departme nt invites you to tell us of any
errors you encounter in this document or to suggest ide as for otherwise
improving it. Please help us better understand what you expect from our
documentation so that we can continuously improve its accuracy and
usability.
We seriously consider every customer comment we receive. You can reach us
at tech_comm@waters.com.
ii
Contacting Waters
Contact Waters® with enhancement requests or techn ical questions regard ing
the use, transportation, removal, or disposal of any Waters prod uct. You can
reach us via the Internet, telephone, or conventional mail.
Waters contact information
Contacting mediumInformation
InternetThe Waters Web site includes phone numbers
for Waters locations worldwi de. Go to
www.waters.com, and click About Waters >
Worldwide Offices.
TelephoneIn the USA or Canada, phone 508 478-2000.
Conventional mailWaters Corporation
34 Maple Street
Milford, MA 01757
USA
iii
Safety considerations
Some reagents and samples used with Waters® instruments ca n po se
chemical, biological, and radiological hazard s. Be sure you are aware of the
potentially hazardous effects of all substances you work with. Always observe
Good Laboratory Practice (GLP) guidelines, published by the U.S. Food and
Drug Administration, and consult your organization’s safety representative
for guidance.
When you develop methods, follow the “Pro tocol for the Ado ption of Analyt ical
Methods in the Clinical Chemistry Laboratory,” Ame rican Journal of Medical Technology, 44, 1, pages 30–37 (1978). This protocol addresses good operating
procedures and the techniques necessary to validate system and method
performance.
Safety advisories
Consult Appendix A for a comprehensive list of warning and caution
advisories.
Operating this detector
When operating this detector, follow standard quality control procedures and
the guidelines presented in this section.
iv
Symbols
P
SymbolDefinition
Intended use
The Waters® 2489 UV/Visible detector can be used for in vitro diagnostic
testing to analyze many compounds, including diagnostic indicators and
therapeutically monitored compounds . However, only professionally trained
and qualified laboratory personnel should use the instrument for those
purposes.
E C RE
Authorized representativ e of the
European Community
Confirms that a manufactured
product complies with all applicable
European Community directives
For in vitro diagnostic use
IV D
The Waters 2489 UV/Visible Detector is CE-marked according to
the European Union In Vitro Diagnostic Device Directive
98/79/EC.
Calibrating the detector
To calibrate the detector, follow acceptable calibration methods using at least
five standards to generate a standard curve . The concentration range for
standards should cover the entire range of quali ty-control samples, typical
specimens, and atypical specimens.
v
Quality control
Routinely run three quality-control samples that represent subnormal,
normal, and above-normal levels of a compound. Ensure that quality-control
sample results fall within an acceptable range, and evaluate precision from
day to day and run to run. Data col lected when qualit y control samples are ou t
of range might not be valid. Do not r eport the se dat a until you ar e cert ain that
the instrument performs satisfactorily.
When analyzing samples from a com plex matrix such as soil, tissue,
serum/plasma, whole blood, and so on, note that the matrix co mponents can
adversely affect results. To minimize these matrix effec ts, Waters
recommends you adopt the following measures:
•Prior to the instrumental analysis, use appropria te sample
pretreatment such as protein precipitation, liquid/liquid extraction
(LLE), or solid phase extraction (SPE) to remove matrix interferences.
•Whenever possible, verify method accuracy and precision using
matrix-matched calibrators and QC samples.
•Use one or more internal standard compounds, preferably isotopically
labeled analytes.
vi
IVD authorized representative
Waters Corp o ra tion (Microm a ss UK Ltd.)
Floats Road
Wythenshawe
Manchester M23 9LZ
United Kingdom
Waters Corporation (Micromass UK
Limited) is registered in the United
Kingdom with the Medicines and
Healthcare Products Regulatory Agency
(MHRA) at Market Towers, 1 Nine Elms
Lane, London, SW8 5NQ. The reference
number is IVD000167.
vii
viii
Table of Contents
1 Theory and Principles of Operation .................................................. 1-1
UV cutoffs for common solvents...................................................................... D-9
Mixed mobile phases...................................................................................... D-10
Wavelength selection for chromophore detection......................................... D-11
xviTable of Contents
1Theory and Principles of
Operation
This chapter summarizes the Waters® 2489 UV/Visible Detector features
and describes the theory and principles of operation.
Contents:
TopicPage
Detector description1-2
Principles of operation1-4
Operational modes1-11
See also: Appendix B for system specifications and Appendix D for
information on high-performance liquid chromatograp hy (HPLC)
solvent considerations.
1-1
Detector description
The Waters 2489 UV/Visible Detector is a two-channel ultraviolet/visible
(UV/Vis) detector designed for high-performance liquid chromatography
(HPLC) applications.
Waters 2489 UV/Visible Detector
Inlet
The detector can oper ate ei ther as a s ta nd-alone unit (w ith a char t record er or
integrator) or as an integral part of a Waters chromatography system.
The detector can be configured with Empower™ or MassLynx™ software
systems.
Features
The detector operates from 190 to 700 nm. The detector uses optics with an
enhanced illumination system for improved performance. These design
features increase the optical throughput and sensitivity and reduce
bandwidth for an overall increase in signal-to-noise ratio and improved
linearity.
1-2Theory and Principles of Operation
The detector has the following capabilities:
•Stand-alone programmability – Stores up to five user- def ined programs
(or methods) consisting of up to 50 programmable timed events and two
threshold events each.
•Single or dual wavelength – Monitors absorbance at one or two discrete
•Automatic second order filter – Automatically engaged for wavelengths
370 nm and greater and removed for wavelengths 369 nm or less.
•Spectrum scan and storage – Supports spectrum scan, display,
subtraction, storage, and playback, in addi tion to standard absorbance
and UV/Vis functionality.
•Cuvette qualification – Facilitates qualification of the detector by
insertion of a standard in a cuvette without breaking any fluid line
connections. Waters qualification kits are available in cuvette form to
support this feature. This feature als o allows you to use the detector as a
benchtop spectrophotometer.
•Cuvette sample analysis – Allows the spectrum of any sample placed in
the cuvette to be recorded.
•Method editing and storage – Supports basic me thod programming,
storage, and retrieval from the front panel.
•Full diagnostic capability – Supports buil t-in diagnostic t ools to optimize
functionality and performance.
•Two contact closure outputs – The detector has two configurable
switches, each of which can accommodate a maximum of +
30 Vdc, 1.2-A
current carry, and 0.5-A current switching. The switches (SW1 and
SW2) can trigger fraction collectors and other external devices, as well
as activate based on time, absorbance threshold, or ratio criteria.
•Improved thermal wander management– To mitigate thermal
instability caused by ambient temperature changes, the detector has
improved insulation (for better air flow acros s the optics bench) and a
variable speed fan that will run at higher or lower speeds as needed.
•Median Baseline Filter (MBF) - A variation of the data mode, t he MBF is
intended to decrease the effects of gradient separations on the
chromatographic baseline. The MBF enhances the UV detector's
baseline stability by decreasing its curvature, making the development
of integration methods easier.
Detector description1-3
Principles of operation
To use the detector effectively, you should be famili ar wit h i ts optical and
electronic design and the theory and principles of its operation.
This section describes the following parts and functions of the detector:
•Optics
•Wavelength verification and test
•Flow cell
•Electronics
Detector optics
The Waters 2489 UV/Visible Detector optics are based on a Fastie-Ebert
monochromator and include the following:
•High brightness deuterium (D
•Two mirrors: one off-axis ellipsoidal mirror and one spherical mirror
•Filter wheel
•Shutter, wavelength calibration filter , and second order filter
•Entrance slit
•Blazed, plane holographic diffraction grating
•Beamsplitter
•Sample and reference photodiodes
•Waters TaperSlit™ Flow Cell (its entrance is the exit slit of the
monochromator)
•Cuvette holder
) lamp
2
1-4Theory and Principles of Operation
Waters 2489 UV/Visible Detector optics assembly
D2 lamp
Filter
wheel
Slit
Grating
TaperSlit
Flow Cell
Beamsplitter
Reference
photodiode
Ellipsoidal
mirror
Sample
photodiode
Window
Optional
cuvette
Spherical
mirror
Optics assembly light path
The detector provides an extremely effic ient design for exceptionally high
light throughput. It operates as follows:
1.The ellipsoidal mirror collects li ght from the lamp and focuses it through
the filter wheel onto the entrance slit. The spherical mirror directs light
toward the grating. A different portion of the spherical mirror focuses
dispersed light of a particular wavelength band, determined by the
grating angle, onto the entrance of the flow cell. Light exiting the flow
cell passes through the cuvette location to the sample photodiode.
2.The beamsplitter, located just ahead of the flow cell, diverts a portion of
the light to a reference photodiode.
3.When you enter a new wavelength through the det ecto r’s f ront pane l (o r
through Empower™ or MassLynx™ softwar e ), the detector rotates the
grating to the appropriate position.
Principles of operation1-5
4.The preamplifier board integrates and digi tizes the currents from the
photodiodes for processing by the signal processing electronics and
output to a computer, chart recorder, or integrator.
Waters TaperSlit Flow Cell
The Waters TaperSlit Flow Cell used in this detector renders the detector
baseline less sensitive to changes in mobile phase refractive index (RI). RI
changes occur during gradient separations or res ult from temperature or
pump-induced pressure fluctuations.
To achieve RI immunity, a combination of a spherical mirror, a lens at the
entrance of the flow cell, and a taper to the internal bore of the flow cell
prevents light rays from striking the internal walls of the flow cell. An
additional feature of the TaperSlit flow cell and the reason for its name is the
shape of the flow cell entrance, which matches the shape of the entrance slit.
The detector achieves higher light throughput for a given spec tral resolution
via the TaperSlit cell design, compared to a conventional flow cell with a
circular entrance.
As shown in the figure below, in a conventional cell, light bends and hits the
wall of the flow cell. Four beams go in, but only two come out. In the Waters
TaperSlit Analytical Cell, the combination of the lens and Taper Slit bore
geometry prevents light from hitting the cell walls. Four beams go in, and four
beams come out.
1-6Theory and Principles of Operation
Comparison of flow cell characteristics
0
Conventional Cell
UV
Light
Window
Waters TaperSlit™
Analytical Cell
UV
Light
Lens
Window
Window
TP0153
The standard analytical, inert, and LC/ MS cells have a path length of 10 mm.
The semi-prep and microbore cell path length is 3 mm. The autopurification
cell path length is 1.0 mm. A variabl e path length flow c ell (path length 0. 15 to
3 mm) is also available.
Filtering noise
The detector provides a Hamming filter to minimize noise. The Hamming
filter is a digital finite impulse response filter, which creates peak height
degradation and enhances the filtering of high frequency noise.
The behavior of the filter depends on the filter time constant you select. You
can program a filter time to be Fast, Slow, Normal, or Other. If you select
Fast, Slow, or Normal, you do not need to enter a value. The filter constant is
determined by the data rate. If you select Other, you can enter a value.
However, the value you enter will be rounded up or down to a value based on
the data rate.
Principles of operation1-7
The filter time constant adjusts the f ilter response time to achieve an optimal
signal-to-noise ratio. Select ing Other and entering a value of 0.0 disables all
filtering.
Lower time constant settings produce these effects:
•Narrow peaks with minimal peak distortion a nd time delay
•Very small peaks become harder to discriminate from baseline noise
•Less baseline noise is removed
Higher time constant settings produce these effects:
•Greatly decrease baseline noise
•Shorten and broaden peaks
The software includes fast or normal filtering cons tants at each data rate that
are appropriate for high speed or high sensitivity applications respectively.
The following figure shows the relationship between increased filter time
constant and absorbance.
1-8Theory and Principles of Operation
Filter Time Constant comparison
Tip: Although the peak shape shows some distortion and the signal output is
delayed with different time constants, the peak area remains the same.
Wavelength verification and test
The detector deuterium arc lamp and the integral erbium filter exhibit peaks
in the transmission spectrum at known wavelengths.
Upon startup, the detector verifies calibration by comparing the locations of
these peaks with expected wavelengt hs based on cali bration data stored in the
detector’s m e m o r y . If th e results of thi s v e ri fication dif fer from the stor ed
calibration by more than 1.0 nm, the detector displays a Wavelength
Verification Failure message. The detector verif ies rather than r ecalibrates on
startup to avoid errors that may occur because of residual material s left i n the
flow cell and /o r the cuvette.
TP02833
Principles of operation1-9
Requirement: Always ensure that the cuvette is removed and the cuvette
holder and front left panel door are secured during startup verification.
You can initiate a manual wavelength calibration at any time. A manual
calibration replaces the previous calibration data with new data. See
“Wavelength calibration” on pag e 3-30 for the manual wavelength calibration
procedure.
The verification and calibration algorithms are virtually iden tical. However,
the verification algorithm may issue an error message indicatin g that actual
data does not match stored data , wher e the calib ration algor ithm rep lace s the
stored data with the new data.
The detector wavelength verification procedures establish an approximate
Home position using a grating homing sensor. Once Home is established, the
detector locates and references the 656. 1-nm peak in the deuterium lamp
emission spectrum.
The integral erbium filter moves into the common light path ahead of the fl ow
cell entrance slit, enabling the detector to locate three additional spectral
features at these wavelengths:
•256.7 nm (UV)
•379.0 nm
•521.5 nm
The verification tests for the det ect or require 5 minutes of lamp warmup time
so the lamp can stabilize.
If you run the detector continuously, Waters recommend s that you perform
wavelength verification weekly by turning off the detect or, then turning it on
again.
See also: “Wavelength calibration” on page 3-30.
1-10Theory and Principles of Operation
Operational modes
The detector operates in single or dual wavelength mode, allows spectrum
scanning using a flow cell or a cuvett e, and provide s RatioPlot , differe nce plot,
and MaxPlot functions.
Single wavelength mode
Single wavelength is the default mode of operation for the detector. The
detector supports monitoring of a single wavelength from 190 nm to 700 nm,
settable in 1-nm increments on channel A. You can configure the analog
outputs for channel B while the detector is operating in single wavelength
mode, so you can use channel B to obtain additional information about the
wavelength selected on channel A.
In single wavelength mode, the detector automatically engages the second
order filter for wavelengths 370 nm and above and removes it for wavelengths
under 370 nm. The second or der filte r is an op tical filt er that bloc ks unwanted
ultraviolet (UV) light from striking the diff raction grating and interfering
with absorbance detection above 370 nm.
You can configure several additional parameters when using the det ector in
single wavelength mode.
Primary parameters
The following are the major parameters you can use in single wavelength
mode:
•Wavelength in nm – Specifies a wavelength for channel A from 190 to
700 nm settable in 1-nm increments.
•Sensitivity in AUFS – Specifies the scaling factor for the analog output
channels and corresponds to the absorbance unit (AU) value where the
analog outputs saturate at full-scale values. Absorbance units full-scale
(AUFS) vary from 0.0001 to 4.000 AU.
Note: Changing the sensitivity (AUFS) setting affects the 2-V output.
•Chart polarity (+ or –) – Reverses the polarity of the charted
chromatogram. Select + for a normal chromatogram, or – for an inverted
chromatogram. This function changes t he direction o f the plot on the 2 -V
output, similar to reversing the leads to an external chart recorder.
Operational modes1-11
•Filter time constant – Programs a filter time in seconds. Options are
Fast, Slow, Normal, or Other. If yo u sele ct Fast, S low, or Nor mal, you d o
not need to enter a value. The filter constant is determined by the data
rate. If you select Other, you can enter a value, but the value you enter
will be rounded up or down to a value based on the data rate. Selecting
Other and entering a value of 0.0 disables all filtering.
•Analog rate – Specifies a value up to 80 Hz.
Secondary parameters
When on the absorbance (or HOME) screen in single wavelength mode,
pressing Next brings you to several pages of these secondary, or less
frequently specified, parameters:
•Absorbance offset (in mV)
•Auto zero on inject
•Auto zero on λ changes
“Primary and secondary functions” on page 3-14 and the Table titled
“Absorbance and message screen icons” on page 3-4 explain the functions,
ranges, and defaults of these parameter s.
Dual wavelength mode
In dual wavelength mode, the detector can monitor two wavelengths, one on
channel A and one on channel B. The sampling frequency is reduced to 1 or
2 Hz, limiting use of this mode to more standard chromatography where peaks
span at least 20 seconds to enable full characterization of a peak. You can use
dual wavelength mode to obtain additional information about an analyte by
running a RatioPlot or a MaxPlot.
The detector allows you to select any two wavelengths from 190 to 700 nm.
In dual wavelength mode, the following conditions apply:
•If both selected wavelengths are greater than 370 nm, the detector
applies the second order filter to block unwanted UV light.
•If both selected wavelengths are less than or equal to 370 nm, the
detector removes the second order filter.
•If the selected wavelengths bracket the 370 nm threshold, the detector
does not apply the second order filter and issues a warning message that
any data collected for the wavelength above 370 nm may contain
1-12Theory and Principles of Operation
inaccuracies because of possible UV light interference (second order
effects).
Chart Out selection modes
When operating in dual wavelength mode, the d etector off ers these c hoices f or
analog output in addition to the selections off ered in single wavelength mode
and explained in “Single wavelength mode” on page 1-11. The default
selection for dual wavelength mode is Absorbance.
•Absorbance (A and B) – This is the standard LC mode where the curr ent
absorption is scaled and sent directly out the analog output. The scaling
depends on the AUFS setting and the absor bance offset. The abs orbance
value is scaled for the 2-V analog output. If a setting of 1 AU/V is
desired, you can set an AUFS of 2.0000 for either the A or B output
channels that can be controlled independently, even in single
wavelength mode.
•MaxPlot – This mode results in the output of the larger of the two
absorbance values, scaled to the selected AUFS sett ing. This mode is
useful when looking at multiple compounds with absorbancies at two
separate wavelengths with one data channel.
•RatioPlot (A/B) – This mode produces the ratio of absorbance from two
wavelengths. Theoretically, the ratio is constant for a pure
chromatographic peak and variable f or an impure peak. This re sults in a
nonsquared response. Instead of a programmable AUFS, the detector
provides minimum and maximum ratio values that scale the ratio plot
proportionally. In addition, a configurable minimum absorbance threshold activates ratio output scaling only when it reaches the
absorbance at both wavelengths.
•Difference Plot (A-B) – This mode plots the arithmetic difference in
absorbance for the two monitored wavelengths.
Spectrum scanning
Note: When the detector is operating under the control of the Empower
software, the scanning function is disabled.
You can use the detector as a spectrophot ometer to acquire spectr a from either
the flow cell or the cuvette. You can scan and store up to three sp ectra (three
reference or zero scans, or three sample scans) in memory f or playback or to
compare with other spectra.
Operational modes1-13
The major difference between the detector and a double-beam
spectrophotometer is that the detector employs only one flow cell or cuvette,
rather than a simultaneous sample and a reference pair.
Recommendation: Use a matched pair of cuvettes for the zero and sample
scans.
The detector obtains an absorbance spectrum by perfor ming two types of scan
on the flow cell or using the cuvette:
•Zero scan – Characterizes the baseline abs orbance spe ctrum of a solvent.
•Sample scan – Subtracts the zero scan, so the results displayed or
charted are of the sample only.
To obtain a spectrum of a sample with the detector, you need to run a zero
scan first, followed by a sample scan. Typ icall y, the zero scan i s run wi th pure
solvent and the sample scan is of the analyte dissolved in that solvent.
Spectra can be simultaneously charted on the channel A output, or acquired
and stored in memory for later playback.
See also: “Scanning using the cuvette” on page 3-59 and “Scanning using a
flow cell and a syringe” on page 3-62.
Cuvette operations
The detector cuvette option is used to measure the absorbance spectrum of a
sample in a cuvette.
To generate and store a spectrum:
1.Acquire a zero scan, which measures the absorbance of the contents of
the cuvette and flow cell over the desired wavelength range.
2.Acquire a sample (absorbance) scan, which measures the absorbance of
the analyte dissolved in mobile phase.
The detector subtracts the zero scan from the sample scan to create a sample
spectrum.
Since the cuvette scan is acquired by measuring the absorbance from a light
path that includes both the flow cell and the cuvet te, the so lvent co ndit ions in
the flow cell should be identical for both scans. For a detailed explanation of
cuvette scanning, see “Scanning using the cuvette” on page 3-59.
1-14Theory and Principles of Operation
Loading...
+ 204 hidden pages
You need points to download manuals.
1 point = 1 manual.
You can buy points or you can get point for every manual you upload.