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    Grimm MiniWRAS 1371粒徑譜儀原版用戶手冊

    The sample air is conducted into the measuring chamber directly from the aerosol intake or through t
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    5 Measurement principle

    The method for detecting airborne particles is based primarily on the particle diameter. Due to the low

    scattered light intensity of ultra-fine particles, the optical detection of particles with a diameter of less

    than approximately 200 nm stops. To cover the widest possible range of particle diameters, here

    ranging from 10 nm to 35μm, the GRIMM MINI-WRAS 1371 combines two measurement methods: the

    electrical detection of ultrafine particles by means of a Faraday cup electrometer in the so-called

    Nano-Sizer and the optical detection of particles with diameters greater than approximately 200 nm by

    measuring the scattered light intensity. The sample air is first passed through the optical aerosol

    spectrometer. Then the particles with a diameter greater than about 2 2μm are separated in order to

    keep the contamination of the subsequent electric sensor as small as possible. The combination of the

    two measurement methods results in a particle size distribution in the range of 10 nm to 35μm in a

    total of 41 size classes.

    5.1 Measurement principle of the optical aerosol spectrometer

    The sample air is conducted into the measuring chamber directly from the aerosol intake or through

    the application-specific sample air collector. Particles contained in the sample air are captured in the

    measuring chamber using light-scattering photometry. The scattered light impulse of each individual

    particle is counted and the intensity of the scattered light signal is assigned to a particle size. The

    measurement principle is shown schematically in Figure 4-1.

    With the 1371-MINI-WRAS, the wavelength is in the visible range of 660 nm. The laser diode can be

    operated in what is known as multiplex mode, which means that the intensity of the laser beam is

    modulated. This allows particles to be detected in a very broad size range from 0.25 μm to 32 μm with

    this model. The laser beam is focused into a flat band by lighting optics. In focus the laser beam

    evenly lights a small sensing volume and is then conducted into a light trap.

    The sample air is aerodynamically focused and conducted through the interior of the sensing volume

    as a particle stream. 

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