
Transverse-Heated Graphite Furnace Atomic Absorption Spectrometer
横向加热石墨炉原子吸收光谱仪
- CE (to be confirmed)
- +2
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同时多元素石墨炉原子吸收光谱仪
Price on request — FOB / CIF quoted per order
Prices depend on configuration, quantity and destination port.
| Simultaneous elements | 2–6 |
|---|---|
| Atomizer | graphite tube, 3000 °C |
| Detection limit | 0.05–2 µg/L typical |
| Optical channels | fixed per element |
| Sample volume | 10–50 µL |
| Background correction | Zeeman effect |
By Lab Manufacturers China Technical TeamLast reviewed Standards: Ph. Eur. 2.2.22 Atomic absorption spectrometry, USP <852> Atomic Absorption Spectroscopy, US EPA Method 7010 Graphite furnace atomic absorption spectrophotometry
A simultaneous multi-element graphite furnace AAS measures several elements from one atomization using multiple lamps and detectors. It is chosen when high sample numbers and short element lists make single-element sequential runs too slow.
A simultaneous multi-element graphite furnace AAS measures several elements from one atomization using multiple lamps and detectors. It is chosen when high sample numbers and short element lists make single-element sequential runs too slow.
This instrument uses a polychromator with several fixed detector channels, each aligned to a different element resonance line, together with a set of hollow-cathode lamps that are modulated so their signals can be separated. One atomization event therefore yields simultaneous absorbance peaks for elements with compatible temperature programs. The approach reduces analysis time and sample consumption substantially for panels such as lead, cadmium, chromium and copper in the same digest, which suits high-volume environmental and food testing. The trade-off is that elements must share a temperature program, and less favorable atomization conditions for some elements may increase detection limits compared with optimized single-element methods. Background correction is usually Zeeman, and software deconvolutes each channel. Careful method development and validation are needed because the shared program constrains each element.
A measured aliquot of sample, typically 5 to 50 microlitres, is deposited into a graphite tube through a dosing hole. The tube is heated in programmed stages: drying to evaporate solvent, pyrolysis to remove organic and inorganic matrix, atomization at high temperature to create a transient cloud of free atoms, and cleaning to remove residue. A hollow-cathode lamp emits the element resonance line through the tube, and the detector records a transient absorbance peak whose area is proportional to the analyte mass. Because atomization is efficient and atoms remain in the optical path longer than in a flame, detection limits are far lower, often in the nanogram per litre range for cadmium and lead. Strong background correction by Zeeman effect or deuterium lamp is essential, and matrix modifiers stabilize analytes during pyrolysis. Tubes and platforms are consumables, and temperature programs are optimized for each matrix.
A typical simultaneous multi-element graphite furnace aas configuration offers simultaneous elements of 2–6, atomizer of graphite tube, 3000 °C, detection limit of 0.05–2 µg/L typical, optical channels of fixed per element, sample volume of 10–50 µL and background correction of Zeeman effect. Values are indicative of the product class; the exact figures for each configuration are confirmed on the quotation and the calibration documents supplied with the instrument.
The Simultaneous Multi-Element Graphite Furnace AAS is used in multi-element panels in water and wastewater, food toxic metal screening panels, clinical trace element panels and high-volume contract trace analysis. Across the wider Graphite Furnace AAS class, laboratories also deploy it for trace metals in drinking water and wastewater, lead and cadmium in food, blood and urine and elemental impurities in pharmaceutical materials.
Relevant standards and methods include Ph. Eur. 2.2.22 Atomic absorption spectrometry, USP <852> Atomic Absorption Spectroscopy, US EPA Method 7010 Graphite furnace atomic absorption spectrophotometry, ISO 15586 Water quality — Determination of trace elements by graphite furnace AAS, ICH Q2(R2) Validation of analytical procedures and IEC 61010-1. Certification candidates for this model are CE, ISO 9001 manufacturing and 21 CFR Part 11 software compliance; each is to be confirmed for the specific configuration before shipment, and certificates are supplied only where they have been issued.
Graphite furnace systems need argon of high purity, a stable power supply, temperature-controlled cooling and adequate exhaust for pyrolysis vapors. Acid digestion or dilution precedes most measurements, and ultrapure reagents and clean vessels are essential because contamination is visible at nanogram per litre levels. Matrix modifiers must be prepared accurately and dosed reproducibly. Operating cost is dominated by graphite tubes, platforms and lamps, so tracking firings and sensitivity helps schedule replacement. Daily checks include autosampler alignment, blank levels and calibration verification. Because each matrix behaves differently, temperature programs require development and should be fixed in the method with defined acceptance criteria.
Select a simultaneous instrument when a fixed panel of compatible elements is measured in large numbers and time per result matters. Confirm that the shared temperature program gives acceptable sensitivity and precision for every element in the panel, and validate each channel separately. If the panel changes often, a single-element sequential system may be more flexible.
Choose a graphite furnace system when trace or ultratrace detection limits are required for a limited number of elements and sample volumes are small. Transverse-heated tubes give more uniform temperature and better reproducibility, while end-heated tubes are simpler and less costly. Zeeman background correction is preferred for complex matrices that produce high structured background. An autosampler with modifier dosing and automatic dilution is important for throughput and for reproducible standard addition. Simultaneous multi-element instruments reduce analysis time when several elements are required, but single-element sequential operation remains the most common and lowest-cost approach. Confirm the graphite tube type and coating suit your elements, since carbide-forming elements such as silicon and vanadium require special tubes.
| Simultaneous elements | 2–6 |
|---|---|
| Atomizer | graphite tube, 3000 °C |
| Detection limit | 0.05–2 µg/L typical |
| Optical channels | fixed per element |
| Sample volume | 10–50 µL |
| Background correction | Zeeman effect |
| Lamp modulation | electronic, per channel |
| Analysis time | 60–150 s for all channels |
| Purge gas | argon, 200–300 mL/min |
| Interface | Ethernet |
Indicative values for this product class. Final specifications are confirmed on the quotation and in the calibration documents supplied with the instrument.
All detected elements atomize during the same furnace firing, so there is only one drying, pyrolysis and atomization sequence. Elements with very different volatilities or matrix requirements cannot each be optimized. Choose panels of elements with compatible behavior, and verify that detection limits remain acceptable for each.
Not necessarily. Sharing a temperature program and splitting lamp energy among channels can raise detection limits compared with a method optimized for one element. The gain is speed and sample economy. For the lowest limits, single-element methods with tailored programs usually remain better.
Each lamp is modulated at a distinct frequency or time slot, and the detector electronics synchronize with it so only the matching signal is recorded. Fixed optical channels isolate the specific resonance lines. Where lines still overlap, software applies correction and the method is validated for cross-talk.
Detection limits are commonly 0.01 to 1 microgram per litre for many elements, with cadmium and lead at the lower end using 20 microlitre injections. Larger injection volumes, preconcentration or a platform can improve limits further. Detection limits depend on matrix, tube condition, lamp and the temperature program used.
Pyrolysis leaves residual matrix that produces high, structured background and smoke during atomization. Zeeman correction measures background very close to the analyte line and handles this structured background well, whereas deuterium correction can be inadequate when background is high or rapidly changing. That is why Zeeman systems dominate difficult matrices.
Optimize drying to avoid spattering, then increase pyrolysis temperature until analyte loss begins, and set atomization as low as possible for a sharp, complete peak without tailing. Cleanout must remove residue without shortening tube life. Modifier choice, observation of peak shape and recovery from spiked samples guide each step.

横向加热石墨炉原子吸收光谱仪


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