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BSA Flow Software Installation and User's Guide - CSI

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This is often not necessary in 1D applications, but for 2D <strong>and</strong> 3D it is<br />

indispensable.<br />

For 1D applications these filters block out background light <strong>and</strong> are<br />

recommended. With He-Ne lasers use filters for wavelength 623.8 nm (red).<br />

With argon lasers use filters for wavelengths 514.5 nm (green), or 488 nm<br />

(blue) or 476.5 nm (violet).<br />

For 2D applications, the 58N71 2D extension kit is installed in the detector<br />

unit. The kit comprises a colour beam splitter, three 514.5 nm interference<br />

filters, one 488 nm interference filter <strong>and</strong> a photo-multiplier.<br />

For 3D applications, the 58N72 2D to 3D extension kit is installed. This kit<br />

comprises a colour beam splitter, a 476.5 nm interference filter <strong>and</strong> a photomultiplier.<br />

If used for 2D or 3D measurement, i.e. with a 58N71 2D extension kit or<br />

(also) a 58N72 3D extension kit installed, the 57X32 filter is required to let<br />

in the green light (wavelength 514.5 nm), while blocking out the light<br />

carrying the other velocity components.<br />

The light from the middle segment of the probe, U3, passes through one (or<br />

two) beam splitters separating out the 488 nm (blue) light, which is directed<br />

to the photo-multiplier tube for the V channel (2D <strong>and</strong> 3D), <strong>and</strong> the 476.5<br />

nm (violet) light, which is received by the photo-multiplier tube for the W<br />

channel (3D).<br />

• DualPDA<br />

For U1 <strong>and</strong> U2 these have a narrow pass b<strong>and</strong> at 514.5 nm wavelength<br />

corresponding to the green argon line. For V1 <strong>and</strong> V2 the interference filters<br />

pass blue light of wavelength 488 nm.<br />

The 58N82 DualPDA Velocity Extension Kit comprises a fifth interference<br />

filter, with a pass b<strong>and</strong> for the 476.5 nm wavelength.<br />

Calibration The electrical response of a photo-multiplier tube lags slightly relative<br />

system to the light input. This lag depends partly on the individual tube <strong>and</strong> partly<br />

on the high voltage applied to the photo-multiplier anode. Lack of<br />

knowledge of the exact value of the difference in delay between channels<br />

U1, U2, V1 <strong>and</strong> V2 could lead to substantial errors in the estimated phase<br />

differences <strong>and</strong> hence to unreliable calculations of the particle diameter.<br />

<strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>:Reference guide 7-49

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