
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
Welcome to Lab Manufacturers China — laboratory instruments direct from a Chinese manufacturer

端部加热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 | end-heated graphite tube |
|---|---|
| Maximum temperature | 2800–3000 °C |
| Heating rate | up to 1500 °C/s |
| Detection limit | 0.01–1 µg/L typical |
| Background correction | deuterium or Zeeman |
| Sample volume | 5–50 µL |
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
An end-heated graphite furnace AAS passes current along the tube length from cooled end contacts. It is the cost-effective choice for routine trace-metal analysis where the most difficult matrices are not required.
An end-heated graphite furnace AAS passes current along the tube length from cooled end contacts. It is the cost-effective choice for routine trace-metal analysis where the most difficult matrices are not required.
In this classic design the tube ends are held in cooled electrode assemblies and current flows along the tube, producing the highest temperature at the center and cooler zones near the ends. It is mechanically simple, uses inexpensive tubes and has a large installed base, making it economical for routine work. The temperature gradient can cause condensation of volatile analytes at the cooler ends, so peak shapes may be slightly broader and memory effects can occur with elements such as cadmium. Careful temperature programming, the use of a platform and matrix modifiers reduce these effects. Deuterium or Zeeman background correction can be fitted, and autosamplers with modifier dosing are widely available. The design suits water, environmental and food testing where matrices are well characterized and detection limits are moderate.
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 end-heated graphite furnace atomic absorption spectrometer configuration offers atomizer of end-heated graphite tube, maximum temperature of 2800–3000 °C, heating rate of up to 1500 °C/s, detection limit of 0.01–1 µg/L typical, background correction of deuterium or Zeeman and sample volume of 5–50 µL. 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 End-Heated Graphite Furnace Atomic Absorption Spectrometer is used in routine trace metals in drinking water, environmental water and soil digests, food lead and cadmium screening and industrial effluent monitoring. 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 an end-heated furnace for routine trace analysis when tube costs, simplicity and a proven design matter more than the ultimate performance on difficult matrices. Specify the elements, detection limits and matrices. If volatile elements or complex samples show memory effects, a transversely heated furnace may be more suitable.
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 | end-heated graphite tube |
|---|---|
| Maximum temperature | 2800–3000 °C |
| Heating rate | up to 1500 °C/s |
| Detection limit | 0.01–1 µg/L typical |
| Background correction | deuterium or Zeeman |
| Sample volume | 5–50 µL |
| Platform | optional |
| Purge gas | argon, 200–300 mL/min |
| Tube life | 200–1000 firings |
| Autosampler positions | 60–120 vials |
Indicative values for this product class. Final specifications are confirmed on the quotation and in the calibration documents supplied with the instrument.
Analyte vapor condenses on the cooler tube ends and is released in later firings, adding to the signal of subsequent samples. Volatile elements such as cadmium are most prone. Higher cleanout temperatures, a platform, matrix modifiers and longer cleaning steps reduce the effect, and blanks between samples detect it.
Yes, end-heated tubes and electrodes are usually cheaper and available from many suppliers, lowering the largest recurring cost in graphite furnace work. However, shorter tube life or higher consumption in some matrices can offset the price advantage, so total cost per determination should be compared.
Methods generally transfer in principle, but temperature programs, modifier levels and atomization conditions must be re-optimized because heating behavior differs. Peak shapes and detection limits may change. Revalidation or at least performance verification is expected before a method is used across furnace designs.
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



