
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)
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直接固体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.
| Sample mass | 0.1–20 mg |
|---|---|
| Atomizer | graphite tube with solid sampler |
| Detection limit | mg/kg range typical |
| Balance resolution | 0.001 mg |
| Maximum temperature | 3000 °C |
| 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 direct solid sampling graphite furnace AAS introduces milligram solid samples into the furnace without digestion. It is chosen to avoid acid digestion, reduce contamination and measure small or difficult-to-dissolve sample materials directly.
A direct solid sampling graphite furnace AAS introduces milligram solid samples into the furnace without digestion. It is chosen to avoid acid digestion, reduce contamination and measure small or difficult-to-dissolve sample materials directly.
This configuration uses a solid sampling accessory, such as a graphite boat, cup or platform, that carries a weighed milligram amount of powder, polymer, biological tissue or food into the furnace. The sample is pyrolyzed and atomized in situ, eliminating the digestion step that causes contamination and analyte loss and consumes time and acids. Calibration is usually performed with solid certified reference materials or by standard addition from solution onto the solid, because the mass-based response differs from liquid injection. The technique is well suited to powders, polymers and materials that are difficult to dissolve, and to laboratories that must avoid hydrofluoric or perchloric acid digestion. Challenges include sample homogeneity, weighing accuracy and matrix variability, so careful method development and replicate measurements are essential.
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 direct solid sampling graphite furnace aas configuration offers sample mass of 0.1–20 mg, atomizer of graphite tube with solid sampler, detection limit of mg/kg range typical, balance resolution of 0.001 mg, maximum temperature of 3000 °C 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 Direct Solid Sampling Graphite Furnace AAS is used in polymer and plastics trace metal screening, powder and ceramic material analysis, biological tissue and food samples and materials difficult to dissolve in acid. 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 IEC 61010-1 safety 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 direct solid sampling when digestion is undesirable, too slow or risks contamination or analyte loss, and when sample masses of a few milligrams are representative. Specify the sample type, expected concentration, required homogeneity and whether solid reference materials exist. Because matrix variability is high, plan replicate measurements and method validation for each material type.
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.
| Sample mass | 0.1–20 mg |
|---|---|
| Atomizer | graphite tube with solid sampler |
| Detection limit | mg/kg range typical |
| Balance resolution | 0.001 mg |
| Maximum temperature | 3000 °C |
| Background correction | Zeeman effect |
| Calibration | solid CRM or solution spiking |
| Purge gas | argon, 200–300 mL/min |
| Temperature program steps | up to 20 |
| Sample throughput | 20–60 per hour |
Indicative values for this product class. Final specifications are confirmed on the quotation and in the calibration documents supplied with the instrument.
Calibration uses solid certified reference materials with matrices similar to the samples, or solution standards spiked onto the solid carrier to build a response curve. Because atomization from a solid differs from liquid injection, matrix-matched solid standards give the best accuracy. Standard addition on the solid is a common alternative.
Typical masses are 0.1 to 20 milligrams, weighed on a microbalance with 0.001 milligram resolution. Small masses reduce matrix load and improve atomization but increase the effect of inhomogeneity, so several replicates are measured. The sample must be ground and homogenized for reproducible results.
Inhomogeneity of the sample, weighing error and variable matrix composition are the main sources. Small samples magnify inhomogeneity, and drying or moisture content shifts the effective mass. Grinding, careful subsampling, moisture correction and replicate measurements control these errors, and calibration with matched solids improves accuracy.
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


高通量自动进样石墨炉原子吸收光谱仪


