Difference between revisions of "JD"

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(Math & Physics)
(Math & Physics)
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<th><math> {J_D} </math></th>
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<th></th>
 
<th>Well in circular drainage area</th>
 
<th>Well in circular drainage area</th>
 
<th>Well in the drainage area with the shape factor <math> {C_A} </math></th>
 
<th>Well in the drainage area with the shape factor <math> {C_A} </math></th>
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<td>Steady state</td>
 
<td>Steady state</td>
 
<td><math> {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{1}{2}+S}} </math></td>
 
<td><math> {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{1}{2}+S}} </math></td>
<td> Calculated with Nodal Analysis using the [[PQplot]] by setting the flowing wellhead pressure (FWHP) equal to the current flowing line pressure (FLP) at the well head. <BR>Use the current value of [[JD]].</td>
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<td> --</td>
  
 
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<td>Pseudo steady state</td>
 
<td>Pseudo steady state</td>
 
<td><math> {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{3}{4}+S}} </math></td>
 
<td><math> {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{3}{4}+S}} </math></td>
<td>Calculated the same way as for the '''Gas Flowing''' case</td>
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<td>--</td>
 
</tr>
 
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Revision as of 11:30, 11 July 2023

Brief

JD - dimensionless productivity index[1], inverse of dimensionless pressure (based on average pressure) which contains the type of flow regime, boundary condition, drainage shape and stimulation [2].

Math & Physics

 {J_D} = \frac{1}{\bar{P}_D}

From the Darcy's law for an unfractured well located in the center of a circular drainage area, the JD is:

Pseudo-steady state:

 {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{3}{4}+S}}

Steady state:

 {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{1}{2}+S}}
Well in circular drainage area Well in the drainage area with the shape factor  {C_A}
Steady state  {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{1}{2}+S}} --
Pseudo steady state  {J_D} = \frac{1}{ln{\frac{r_e}{r_w}-\frac{3}{4}+S}} --

Oil

 {J_D} = \frac{141.2 B \mu}{kh} \frac{q}{\bar{P} - P_{wf}} = \frac{141.2 B \mu}{kh} J
 {q} = \frac{kh}{141.2 B \mu} (\bar{P} - P_{wf}) J_D

Gas

J_D=\frac{1422 \times 10^3\ T_R}{kh} \frac{q_g}{P_{\bar{P}}-P_{P_{wf}}}

Maximum J_D

The undamaged unstimulated vertical well potential in a pseudo steady radial flow is:

 {J_D}_{max} \approx \frac{1}{ln{\frac{500}{0.1}-\frac{3}{4}+0}} \approx 0.13

The maximum possible stimulated well potential for pseudo steady linear flow is:

{J_D}_{max}= \frac{6}{\pi} \approx 1.91 , see 6/π stimulated well potential

The maximum possible stimulated well potential for steady state linear flow is:

{J_D}_{max}= \frac{4}{\pi} \approx 1.27 , see 4/π stimulated well potential

Nomenclature

 B = formation volume factor, bbl/stb
 J = productivity index, stb/psia
 J_D = dimensionless productivity index, dimensionless
 kh = permeability times thickness, md*ft
 \bar{P} = average reservoir pressure, psia
 \bar{P}_D = dimensionless pressure (based on average pressure), dimensionless
 P_{\bar{P}} = average reservoir pseudopressure, psia2/cP
 P_{wf} = well flowing pressure, psia
 P_{P_{wf}} = average well flowing pseudopressure, psia2/cP
 q = flowing rate, stb/d
 q_g = gas rate, MMscfd
 r_w = wellbore radius, ft
 r_e = drainage radius, ft
 S = skin factor, dimensionless
 T = temperature, °R

Greek symbols

 \mu = viscosity, cp

See Also

References

  1. Rueda, J.I.; Mach, J.; Wolcott, D. (2004). "Pushing Fracturing Limits to Maximize Producibility in Turbidite Formations in Russia"Free registration required (SPE-91760-MS). Society of Petroleum Engineers. 
  2. Cite error: Invalid <ref> tag; no text was provided for refs named DW