|
|
Line 1: |
Line 1: |
| In [[fluid statics]], '''capillary pressure''' is the difference in [[pressure]] across the interface between two [[immiscible]] fluids, and thus defined as
| | Hi there. Let [http://www.seekavideo.com/playlist/2199/video/ real psychics] me begin by introducing the writer, her title is Sophia. To perform lacross is something he would never give up. Distributing manufacturing is how he tends to make a living. Some time in the past she chose to reside in Alaska and her mothers and fathers reside close by.<br><br>Take a look at my [http://www.octionx.sinfauganda.co.ug/node/22469 best psychic readings] site: free psychic [[http://www.aseandate.com/index.php?m=member_profile&p=profile&id=13352970 Privacy of Data: This tool is built-with and functions-in Client Side JavaScripting, so only your computer will see or process your data input/output.a cool way to improve]] |
| :<math>p_c=p_{\text{non-wetting phase}}-p_{\text{wetting phase}}</math> | |
| In oil-water systems, water is typically the [[wetting]] phase, while for gas-oil systems, oil is typically the wetting phase.
| |
| | |
| The [[Young–Laplace equation]] states that this pressure difference is proportional to the [[interfacial tension]], <math>\gamma</math>, and inversely proportional to the effective radius, <math>r</math>, of the interface, it also depends on the [[contact angle|wetting angle]], <math>\theta</math>, of the liquid on the surface of the capillary.
| |
| :<math>p_c=\frac{2\gamma \cos \theta}{r}</math>
| |
| | |
| The equation for capillary pressure is only valid under capillary equilibrium, which means that there can not be any flowing phases.
| |
| | |
| == In porous media==
| |
| In [[porous media]], capillary pressure is the force necessary to squeeze a hydrocarbon droplet through a pore throat (works against the interfacial tension between oil and water phases) and is higher for smaller pore diameter. The expression for the capillary pressure remains as before, ''i.e.,''
| |
| <math>p_c=p_{\text{non-wetting phase}}-p_{\text{wetting phase.}}</math> | |
| However, the quantities <math>p_c</math>, <math>p_{\text{non-wetting phase}}</math> and <math>p_{\text{wetting phase}}</math> are quantities that are obtained by averaging these quantities within the pore space of porous media either statistically or using the volume averaging method.<ref>Jacob Bear: “Dynamics of Fluids in Porous Media,” Dover Publications, 1972.</ref>
| |
| | |
| The Brooks-Corey correlation<ref>Brooks, R.H. and Corey, A.T.: “Hydraulic properties of porous
| |
| media,” Hydraulic paper no. 3, Colorado State University, 1964.</ref> for capillary pressure reads
| |
| :<math>p_c = cS_w^{-a}</math>
| |
| where <math>c</math> is the entry capillary pressure, <math>1/a</math> is the pore-size distribution index and <math>S_w</math> is the normalized water saturation (see [[Relative permeability]])
| |
| | |
| ==See also==
| |
| * [[Capillary action]]
| |
| * [[Capillary number]]
| |
| * [[Disjoining pressure]]
| |
| * [[Leverett J-function]]
| |
| * [[Young–Laplace equation]]
| |
| * [[Amott test]]
| |
| * [[Laplace pressure]]
| |
| | |
| ==References==
| |
| * Kim Kinoshita, Electrochemical Oxygen Technology p139, John Wiley & Sons, Inc. 1992.
| |
| * [http://www.articleworld.org/index.php/Capillary_pressure Capillary pressure equations]
| |
| {{reflist}}
| |
| | |
| [[Category:Fluid dynamics]]
| |
| | |
| | |
| {{fluiddynamics-stub}}
| |
Hi there. Let real psychics me begin by introducing the writer, her title is Sophia. To perform lacross is something he would never give up. Distributing manufacturing is how he tends to make a living. Some time in the past she chose to reside in Alaska and her mothers and fathers reside close by.
Take a look at my best psychic readings site: free psychic [Privacy of Data: This tool is built-with and functions-in Client Side JavaScripting, so only your computer will see or process your data input/output.a cool way to improve]