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Portable Diesel Analysis with mid-FTIR
Features
- Cetane number (correlation to ASTM D613)
- Cetane Index (correlation to ASTM D976)
- Cetane Improver
- Total Aromatics (correlation to ASTM D5186)
- FAME (Biodiesel) content in Diesel Fuel (EN 14078)
- Polynuclear Aromatics (correlation to ASTM D5186)
- Built-In Anton Paar Density Meter to convert the concentration of substances from volume% to mass%
- Temperature control
- Small sample volume: 7ml
- No sample preparation: just insert filling tube in sample bottle and press RUN
- Measuring time: 3 minutes
- Fully automated: sample introduction, measurement ...
- No complex technical training required
- Fast and easy on-site calibration of the correlation library in less than 4 minutes/sample
- Optional 6-position sampler
- PC/printer interface
- MINIWIN PC software
- Portable for field applications (optional vehicle battery connector)
ONLY 3 MINUTES FOR A COMPLETE DIESEL ANALYSIS
| Parameter |
Range |
Repeatability |
Standard Deviation (SD, RMSEC) |
| Cetane Number |
25 - 75 |
0.8 |
0.6 - 0.9 |
| Cetane Index |
30 - 70 |
0.4 |
0.4 - 0.6 |
| Cetane Improver |
0 – 5000 ppm |
- |
90 ppm |
| Total Aromatics |
0 – 60 wt. % |
0.5 (@25%) |
0.4 |
| Poly Nuclear Aromatics |
0 – 40 wt. % |
0.4 (@5%) |
0.3 |
| FAME (Biodiesel) in Diesel Fuel |
0 – 40 wt. % |
- |
0.2 (@5 v%), 0.5 (@10 v%) |
| EN 14078 - FAME (Biodiesel) in Diesel Fuel |
0 - 30 v % |
- |
0.3 |
| Distillation Rroperties |
T85, T90, T95 |
- |
- |
| Density @ Room Temp. |
0.500 - 1,999 g/cm3 |
±0.001 g/cm3 |
±0.0005 g/cm3 |
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Technical Data
Display |
large graphics display, backlit |
| Warm-Up Time |
10 min. |
| Response Time |
3 min. |
| Communication |
RS-232 serial port for PC & printer |
| Power Requirements |
100/110/230/240 V AC, 50/60 Hz, 65 W |
| Field Application |
12 V/4A DC (vehicle battery) |
| W x H x D |
200 x 320 x 220 mm (7.9" x 12.6" x 8.7") |
| Weight |
11 kg (24 lb) |
Options & Accessories:
Printer and PC recommended, MINIWIN IROX software: results data storage, upload/download spectra of interest, view IR-spectra graphics ...
Principle
The light of an infrared source (1) is collimated by the mirror (2) and is divided into two equivalent beams with the beamsplitter (3). One beam is reflected by the fixed mirror (4) and the second beam is reflected by the scanning mirror (5). Both beams are recombined in the beamsplitter and travel through the measuring cell (6), which is filled with the unknown sample. The combined beam is collimated onto the infrared-detector (8). The two beams can interfere after the beamsplitter and make a constructive interference for all wavelengths if the two path lengths are equal. If the scanning mirror is shifted, constructive interference is possible only for a wavelength which is a multiple of the shift. The intensity on the detector varies like the cosine-Fourier transform of the spectrum. This values are stored for later evaluation. Performing a Fourier-transform of the stored values after the scan, the absorption spectrum of the unknown mixture is evaluated. The concentration of the various components is calculated using a matrix transformation of 962 x 32 points.
Continuous product development may make it necessary to change product specifications without notice. |