Question:

A circular shaped reservoir has an external radius \(r_e\). A well of radius \(r_w\) lies at the centre of the reservoir. The part of the reservoir around the wellbore, up to a radius \(r_s\), is damaged due to drilling and completion operations, where \(r_w < r_s < r_e\). This formation damage causes an additional pressure drop, \(\Delta p(r)\), that varies with the radial distance \(r\) from the well. Which of the following statements is TRUE about the additional pressure drop at the radial location \(r_s\) due to the formation damage?

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The additional pressure drop caused by damage is confined entirely within the damaged ring and dies out at its outer edge, \(r_s\).
Updated On: Jul 28, 2026
  • \(\Delta p(r_s) = \Delta p(r_w)\)
  • \(\Delta p(r_s) = 0\)
  • \(\Delta p(r_s) = 2\,\Delta p(r_w)\)
  • \(\Delta p(r_s) = 4\,\Delta p(r_w)\)
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The Correct Option is B

Solution and Explanation

Step 1: Understand where the extra pressure drop comes from:
A damaged well has lower permeability in the ring of rock between \(r_w\) and \(r_s\) compared with the rest of the reservoir. Fluid moving through this ring loses more energy than it would if the whole reservoir had the undamaged permeability. This extra energy loss shows up as an additional pressure drop \(\Delta p(r)\), defined as the difference between the actual pressure profile and the pressure profile that would exist if there were no damage at all.
Step 2: Identify the region where this additional drop exists:
Since the rock beyond \(r_s\) has the same, undamaged permeability that is used as the reference for \(\Delta p(r)\), no extra resistance is offered to flow once the fluid is outside the damaged ring. So the additional pressure drop can only build up inside the damaged ring, that is for \(r_w \le r \le r_s\). It is largest at the wellbore face \(r = r_w\), because the fluid has crossed the full thickness of the damaged ring by the time it reaches the well, and it becomes progressively smaller as \(r\) moves outward toward \(r_s\), since less of the damaged ring remains ahead of the flowing fluid.
Step 3: Apply the condition at \(r = r_s\), the outer edge of the damage:
At \(r = r_s\) the fluid has not yet entered the damaged ring, so it has not experienced any of the extra flow resistance caused by the damage. This means the additional pressure drop must be zero exactly at \(r_s\), and it accumulates only as the fluid moves further inward, reaching its full value \(\Delta p(r_w) = \dfrac{141.2\,qB\mu}{kh}\,S\) at the wellbore face, where S is the skin factor.
Step 4: Rule out the remaining options:
Option A claims \(\Delta p(r_s) = \Delta p(r_w)\), which would mean the full skin effect is already present at the outer boundary of the damaged zone, contradicting the fact that the drop builds up from zero at \(r_s\) to a maximum at \(r_w\). Options C and D claim \(\Delta p(r_s)\) is two or four times \(\Delta p(r_w)\), which is impossible since \(\Delta p(r_w)\) is the maximum value of this additional drop and \(\Delta p(r)\) decreases monotonically as \(r\) increases from \(r_w\) to \(r_s\), never exceeding the wellbore value.
Final Answer:
\[ \boxed{\Delta p(r_s) = 0} \]
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