Effective Speed:
~8 L/s
Remaining: 0 / 0
Effective Speed:
~2 L/s
Remaining: 0 / 0
Key Insight
In molecular flow, conductance depends on the cube of the diameter and is inversely proportional to length. A narrower, longer foreline with bends dramatically reduces effective pumping speed at the chamber.
About this animation: Both chambers start with the same number of molecules so evacuation times are directly comparable. Molecule sizes and chamber dimensions are simplified for clarity — focus on the relative evacuation rates, not absolute counts. In viscous flow, molecules follow a parabolic velocity profile (Poiseuille flow — fastest at the centre, stationary at the walls). In molecular flow, molecules travel in straight lines between wall collisions and re-emit in a random direction weighted by Knudsen’s cosine law. The narrow foreline’s smaller bore, greater length, and two 90° bends cause significantly more backscatter in molecular flow, dramatically reducing effective pumping speed at the chamber. This is a 2D cross-section view — in a real cylindrical pipe, wall collisions occur much more frequently (roughly every pipe diameter), producing shorter hops and even greater backscatter in molecular flow than shown here.