For cyclone removal of particulate matter from air, a smaller body diameter gives a stronger vortex and a lower cut size, while a larger body, a wider inlet or a wider gas outlet does the opposite. When one large unit cannot reach the required d50, the flow is split among many small tubes in a multiclone. Multiclones reach 80–95% capture of 5 µm particles. The trade-offs are uneven gas distribution between tubes, backflow through the shared hopper and plugging of narrow tubes by sticky material.
Inlet velocity raises capture up to a limit. Typical design values lie around 15–25 m/s (50–80 ft/s). Kalen and Zenz showed that above about 1.36 times the saltation velocity, collected particles are picked up from the wall again; they put the optimum near 1.25 times that value.
The price of velocity is pressure drop. The Shepherd–Lapple correlation gives ΔP = K·(HW/De²)·(ρgVi²/2), with K = 16 for a plain tangential inlet and De as the outlet diameter. For the example unit this is 6.4 velocity heads, or 3.5 in. w.g. at 15 m/s. At 20 m/s ΔP climbs to 6.2 in. w.g., 78% higher, while d50 improves only from 3.9 to 3.4 µm, since cut size scales with the inverse square root of velocity.