
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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高通量自动进样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.
| Atomizer | graphite tube, 3000 °C |
|---|---|
| Cycle time | 60–120 s per element |
| Sample volume | 5–50 µL |
| Autosampler positions | 60–180 vials |
| Dilution | automatic, up to 100:1 |
| Standard addition | automatic in-tube |
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
This graphite furnace AAS pairs a fast furnace with an autosampler that doses sample, modifier and diluent automatically. It is well chosen for laboratories running many routine trace determinations with standard addition procedures.
This graphite furnace AAS pairs a fast furnace with an autosampler that doses sample, modifier and diluent automatically. It is well chosen for laboratories running many routine trace determinations with standard addition procedures.
Throughput in graphite furnace work is limited by heating cycle time and by manual preparation of modifiers and dilutions. This configuration addresses both by using fast temperature ramps, shortened drying and cleanout steps, and an autosampler that mixes sample with modifier and diluent directly in the tube. Automatic standard addition builds the calibration into each sample aliquot, which compensates for matrix effects without separate spiking by the operator. Vial capacity of 60 to 180 positions and intelligent scheduling allow long unattended runs, while software applies QC rules, automatic reanalysis and dilution factors. Zeeman or deuterium background correction handles residual matrix from the shortened pyrolysis. Typical cycle times are 60 to 120 seconds per element, and the system is widely used for elemental impurity testing, environmental monitoring and contract analysis.
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 high-throughput graphite furnace aas with autosampler and modifier dosing configuration offers atomizer of graphite tube, 3000 °C, cycle time of 60–120 s per element, sample volume of 5–50 µL, autosampler positions of 60–180 vials, dilution of automatic, up to 100:1 and standard addition of automatic in-tube. 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 High-Throughput Graphite Furnace AAS with Autosampler and Modifier Dosing is used in pharmaceutical elemental impurity routine testing, high-volume environmental trace metals, contract laboratory lead and cadmium analysis and food and beverage compliance programs. 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 this configuration when sample numbers are high, matrix effects require standard addition and unattended operation is valuable. Specify the elements, expected concentration ranges, vial capacity and data system requirements. Confirm that cycle time, carry-over and dilution accuracy meet your lowest reporting limits.
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.
| Atomizer | graphite tube, 3000 °C |
|---|---|
| Cycle time | 60–120 s per element |
| Sample volume | 5–50 µL |
| Autosampler positions | 60–180 vials |
| Dilution | automatic, up to 100:1 |
| Standard addition | automatic in-tube |
| Detection limit | 0.01–1 µg/L typical |
| Background correction | Zeeman or deuterium |
| QC functions | blank, spike, duplicate, drift |
| Interface | Ethernet / USB |
Indicative values for this product class. Final specifications are confirmed on the quotation and in the calibration documents supplied with the instrument.
The autosampler adds the sample plus several increasing volumes of a standard into the same tube, and the instrument measures each. The response is extrapolated back to zero addition to give the original concentration. This corrects for matrix effects without preparing separate spiked samples manually.
Each determination requires a full heat cycle for drying, pyrolysis, atomization and cleaning, so cycle time sets the upper limit. Shortening steps risks incomplete drying, matrix build-up or carry-over. Faster ramps, efficient cleanout and overlap with autosampler preparation improve throughput without harming quality.
Yes, with sufficient vial capacity, argon supply, waste handling and stable power, the autosampler can run long sequences unattended. The software should pause or flag when QC criteria fail or gas pressure drops. Review the sequence and blanks before leaving, and confirm data integrity rules are enabled.
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





难熔元素一氧化二氮-乙炔火焰原子吸收光谱仪