Generation of nano-scale test aerosols through condensation

The DNP digital 3000 aerosol generator generates a jump spark between two graphite electrodes under high voltage. The jump spark rips tiny amounts of graphite from the electrodes at high temperatures. The graphite vaporized by this spark then condenses to form highly tiny particles. The high number concentration can result in the coagulation of these very small particles into agglomerates. The aerosol can be diluted by adding mixed air, enabling the defined adjustment of the agglomerate formation. The generated aerosol distribution is very similar to the distribution of diesel soot particles from a combustion engine. The energy converted in each spark remains constant due to the continual spark over voltage. This continuous energy in each spark guarantees stable particle size distribution (see Fig. 1). A technically sophisticated control of the distance between the electrodes during burn-off ensures very high long-term stability. The mass flow can be quickly and easily adjusted within a wide range using the spark frequency (see Fig. 2).

The digital regulation of the frequency and the continuous regulation of the voltage guarantee a more specific regulation of the distance between the two electrodes. This enables a higher constancy of the particle size distribution and the mass flow. Furthermore, every single spark can be regulated, and the energy of the single spark can be determined in principle. An AK protocol for an Ethernet connection via UDP protocol is part of the delivery.

Due to its easy startup, excellent reproducibility, and high functional reliability, the DNP digital 3000 is exceptionally well suited for calibrating particle measurement devices. Because of the superb reproducibility and easy handling, the DNP digital 3000, combined with the REF 3000 reference exhaust, successfully calibrates the PMP measurement chain in the particle measurement program.

Carrier gas: Nitrogen or Argon

Fig. 1: Size distributions of the particle agglomerates at various spark frequencies

Fig. 2: Particle mass flow of the DNP digital 2000 as a function of the spark frequency