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. Author manuscript; available in PMC: 2015 Mar 1.
Published in final edited form as: J Math Biol. 2013 Mar 26;68(4):1023–1049. doi: 10.1007/s00285-013-0667-5

Fig. 2.

Fig. 2

Schematic representation of model TGF system. Hydrodynamic pressure Po(t) = P(0, t) drives flow into loop entrance (x = 0) at time t. Oscillations in inflow pressure result in oscillations in loop pressure P(x, t), flow rate Q(x, t), water flux Φ(x, t), radius R(x, t), and tubular fluid chloride concentration C(x, t).