Figure 9
From: Effects of an imposed axial flow on a Ferrofluidic Taylor-Couette flow
Variation in angular momentum and dimensionless torque. (I) Variation of angular momentum \(L(r)=r{\langle v(r)\rangle }_{\theta ,z}/{R}{{e}}_{i}\) and (II) variation of the dimensionless torque \(G=\nu {J}^{\omega }\) versus the radius r for solutions with increasing Re as indicated in axial and transverse magnetic field at (a) \(R{e}_{i}=110\) and (b) \(R{e}_{i}=270\). The insets in (II) show the variation of the total torque Gtotal for different Re.
