The Microfluidic Blood Cell Counter · AI Generator #GEN-8AA46D19

Physics · fluid-mechanics

Problem

Modern medical devices use microfluidic channels to count blood cells by measuring pressure changes as cells pass through narrow constrictions. Consider a simplified model of such a device: A horizontal microfluidic channel has a wide section of cross-sectional area A1=400  μm2A_1 = 400\;\text{μm}^2 connected to a narrow constriction of area A2=100  μm2A_2 = 100\;\text{μm}^2. Blood plasma (viscosity η=1.2×10−3  Pa⋅s\eta = 1.2 \times 10^{-3}\;\text{Pa·s}, density ρ=1025  kg/m3\rho = 1025\;\text{kg/m}^3) flows through the channel at a steady volumetric flow rate Q=2.0×10−15  m3/sQ = 2.0 \times 10^{-15}\;\text{m}^3\text{/s}. When a spherical red blood cell of diameter d=7.0  μmd = 7.0\;\text{μm} enters the constriction, it completely blocks the narrow section, forcing all fluid to flow around it through an effective annular area. The cell moves through the constriction with the same speed as the fluid would have in that section without obstruction. During the time the cell blocks the constriction, what is the pressure difference between the wide section and the exit of the constriction? Assume the channel length from wide section to constriction exit is L=50  μmL = 50\;\text{μm}, and treat the flow as laminar with the cell creating a uniform annular flow region. Note: For laminar flow through a channel, the pressure drop follows ΔP=32ηLQπd4\Delta P = \frac{32\eta LQ}{\pi d^4} for circular cross-sections of diameter dd.

Related theory

Browse the problem library