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Fluid flow with fluid pressure  p(t, {\bf r}) linearly changing in time:

p(t, {\bf r}) = \psi({\bf r}) + A \cdot t, \quad A = \rm const

The fluid temperature   T(t, {\bf r}) is supposed to vary slowly enough to provide quasistatic equilibrium.


The fluid velocity  {\bf u}(t, {\bf r})  may not be stationary.

In the most general case (both reservoir and pipelines) the fluid motion equation is of fluid pressure and pressure gradient:

(1) {\bf u}(t, {\bf r})= F({\bf r}, p, \nabla p)

with right side dependent on time through the pressure variation.


In case of the flow with velocity dependent on pressure  gradient only {\bf u} = {\bf u}({\bf r}, \nabla p)) the PSS flow velocity will be stationary as the right side of (1) is not dependant on time.


In terms of Well Flow Performance the PSS flow means:

(2) q_t(t) = \rm const
(3) \Delta p(t) = | p_e(t) - p_{wf}(t) | = \Delta p = \rm const

During the PSS regime the formation pressure also declines linearly with time:  p_e(t) \sim t.


The exact solution of diffusion equation for PSS:

(4) p_e(t) = p_i - \frac{q_t}{ V_{\phi} \, c_t} \ t


varying formation pressure at the external reservoir boundary


(5) p_{wf}(t) = p_e(t) - J^{-1} q_t


varying bottom-hole pressure


(6) J = \frac{q_t}{2 \pi \sigma} \left[ \ln \left ( \frac{r_e}{r_w} \right) +S + 0.75 \right]


constant productivity index


and develops a unit slope on PTA diagnostic plot  and Material Balance diagnostic plot:

Fig. 1. PTA Diagnostic Plot for vertical well in single-layer homogeneous reservoir with impermeable circle boundary (PSS).

Pressure is in blue and log-derivative is in red.


See Also


Petroleum Industry / Upstream /  Production / Subsurface Production / Field Study & Modelling / Production Analysis / PSS Diagnostics

Steady State (SS) fluid flow ]




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