To demonstrate Bernoulli's principle, an instructor arranges two circular horizontal plates of radii \( b \) each with distance \( d \) (\( d \ll b \)) between them (see figure). The upper plate has a hole of radius \( a \) in the middle. On blowing air at a speed \( v_0 \) through the hole so that the flow rate of air is \( \pi a^2 v_0 \), it is seen that the lower plate does not fall. If the density of air is \( \rho \), the upward force on the lower plate is well approximated by the formula (assume that the region with \( r<a \) does not contribute to the upward force and the speed of air at the edges is negligible): 