In fluid statics, capillary pressure (${\displaystyle {p_{c}}}$) is the pressure between two immiscible fluids in a thin tube (see capillary action), resulting from the interactions of forces between the fluids and solid walls of the tube. Capillary pressure can serve as both an opposing or driving force for fluid transport and is a significant property for research and industrial purposes (namely microfluidic design and oil extraction from porous rock). It is also observed in natural phenomena.

Capillary pressure is defined as:

${\displaystyle p_{c}=p_{\text{non-wetting phase}}-p_{\text{wetting phase}}}$

where:

${\displaystyle p_{\text{c}}}$is the capillary pressure

${\displaystyle p_{\text{non-wetting phase}}}$ is the pressure of the non-wetting phase

${\displaystyle p_{\text{wetting phase}}}$ is the pressure of the wetting phase

The wetting phase is identified by its ability to preferentially diffuse across the capillary walls before the non-wetting phase. The "wettability" of a fluid depends on its surface tension, the forces that drive a fluid's tendency to take up the minimal amount of space possible, and it is determined by the contact angle of the fluid.^[1] A fluid's "wettability" can be controlled by varying capillary surface properties (e.g. roughness, hydrophilicity). However, in oil-water systems, water is typically the wetting phase, while for gas-oil systems, oil is typically the wetting phase.^[1] Regardless of the system, a pressure difference arises at the resulting curved interface between the two fluids.^[2]

Capillary pressure formulas are derived from the pressure relationship between two fluid phases in a capillary tube in equilibrium, which is that force up = force down. These forces are described as:^[1]

${\displaystyle {\text{force up = interfacial tension of the fluid(s) acting along the perimeter of the capillary tube}}}$

${\displaystyle {\text{force down = (density gradient difference) x (cross-sectional area) x (height of the capillary rise in the tube)}}}$

These forces can be described by the interfacial tension and contact angle of the fluids, and the radius of the capillary tube. An interesting phenomena, capillary rise of water (as pictured to the right) provides a good example of how these properties come together to drive flow through a capillary tube and how these properties are measured in a system. There are two general equations that describe the force up and force down relationship of two fluids in equilibrium.

The Young–Laplace equation is the force up description of capillary pressure, and the most commonly used variation of the capillary pressure equation:^[2][1]

${\displaystyle p_{c}={\frac {2\gamma \cos \theta }{r_{c}}}}$

where:

${\displaystyle \gamma }$ is the interfacial tension

${\displaystyle r}$ is the effective radius of the interface

${\displaystyle \theta }$ is the wetting angle of the liquid on the surface of the capillary

The force down formula for capillary pressure is seen as:^[1]

${\displaystyle p_{c}={\frac {\pi r^{2}h(\Gamma _{w}-\Gamma _{nw})}{\pi r^{2}}}=h(\Gamma _{w}-\Gamma _{nw})}$

where:

${\displaystyle h}$ is the height of the capillary rise

${\displaystyle \Gamma _{w}}$ is the density gradient of the wetting phase

${\displaystyle \Gamma _{nw}}$ is the density gradient of the non-wetting phase

Microfluidics is the study and design of the control or transport of small volumes of fluid flow through porous material or narrow channels for a variety of applications (e.g. mixing, separations). Capillary pressure is one of many geometry-related characteristics that can be altered in a microfluidic device to optimize a certain process. For instance, as the capillary pressure increases, a wettable surface in a channel will pull the liquid through the conduit. This eliminates the need for a pump in the system, and can make the desired process completely autonomous. Capillary pressure can also be utilized to block fluid flow in a microfluidic device.

The capillary pressure in a microchannel can be described as:

${\displaystyle p_{c}=-\gamma \left({\frac {cos\theta _{b}+cos\theta _{t}}{d}}+{\frac {cos\theta _{l}+cos\theta _{r}}{w}}\right)}$

where:

${\displaystyle {\gamma }}$ is the surface tension of the liquid

${\displaystyle {\theta _{b}}}$ is the contact angle at the bottom

${\displaystyle {\theta _{t}}}$ is the contact angle at the top

${\displaystyle {\theta _{l}}}$ is the contact angle at the left side of the channel

${\displaystyle {\theta _{r}}}$ is the contact angles at the right side of the channel

${\displaystyle {d}}$ is the depth

${\displaystyle {w}}$ is the width

Thus, the capillary pressure can be altered by changing the surface tension of the fluid, contact angles of the fluid, or the depth and width of the device channels. To change the surface tension, one can apply a surfactant to the capillary walls. The contact angles vary by sudden expansion or contraction within the device channels. A positive capillary pressure represents a valve on the fluid flow while a negative pressure represents the fluid being pulled into the microchannel.^[3]

Methods for taking physical measurements of capillary pressure in a microchannel have not been thoroughly studied, despite the need for accurate pressure measurements in microfluidics. The primary issue with measuring the pressure in microfluidic devices is that the volume of fluid is too small to be used in standard pressure measurement tools. Some studies have presented the use of microballoons, which are size-changing pressure sensors. Servo-nulling, which is historically used for measuring blood pressure, has also been demonstrated to provide pressure information in microfluidic channels with the assistance of a LabVIEW control system. Essentially, a micropipette is immersed in the microchannel fluid and is programmed to respond to changes in the fluid meniscus. A displacement in the meniscus of the fluid in the micropipette induces a voltage drop, which triggers a pump to restore the original position of the meniscus. The pressure exerted by the pump is interpreted as the pressure within the microchannel.^[4]

Current research in microfluidics is focused on developing point-of-care diagnostics and cell sorting techniques (see lab-on-a-chip), and understanding cell behavior (e.g. cell growth, cell aging). In the field of diagnostics, the lateral flow test is a common microfluidic device platform that utilizes capillary forces to drive fluid transport through a porous membrane. The most famous lateral flow test is the take home pregnancy test, in which bodily fluid initially wets and then flows through the porous membrane, often cellulose or glass fiber, upon reaching a capture line to indicate a positive or negative signal. An advantage to this design, and several other microfluidic devices, is its simplicity (for example, its lack of human intervention during operation) and low cost. However, a disadvantage to these tests is that capillary action cannot be controlled after it has started, so the test time cannot be sped up or slowed down (which could pose an issue if certain time-dependent processes are to take place during the fluid flow).^[5]

Another example of point-of-care work involving a capillary pressure-related design component is the separation of plasma from whole blood by filtration through porous membrane. Efficient and high-volume separation of plasma from whole blood is often necessary for infectious disease diagnostics, like the HIV viral load test. However, this task is often performed through centrifugation, which is limited to clinical laboratory settings. An example of this point-of-care filtration device is a packed-bed filter, which has demonstrated the ability to separate plasma and whole blood by utilizing asymmetric capillary forces within the membrane pores.^[6]

Capillary pressure plays a vital role in extracting sub-surface hydrocarbons (such as petroleum or natural gas) from underneath porous reservoir rocks. Its measurements are utilized to predict reservoir fluid saturations and cap-rock seal capacity, and for assessing relative permeability (the ability of a fluid to be transported in the presence of a second immiscible fluid) data.^[7] Additionally, capillary pressure in porous rocks has been shown to affect phase behavior of the reservoir fluids, thus influencing extraction methods and recovery.^[8] It is crucial to understand these geological properties of the reservoir for its development, production, and management (e.g. how easy it is to extract the hydrocarbons).

^{[dubious – discuss]}The Deepwater Horizon oil spill is an example of why capillary pressure is significant to the petrochemical industry. It is believed that upon the Deepwater Horizon oil rig’s explosion in the Gulf of Mexico in 2010, methane gas had broken through a recently implemented seal, and expanded up and out of the rig. Although capillary pressure studies (or potentially a lack thereof) do not necessarily sit at the root of this particular oil spill, capillary pressure measurements yield crucial information for understanding reservoir properties that could have influenced the engineering decisions made in the Deepwater Horizon event.^[9]

Capillary pressure, as seen in petroleum engineering, is often modeled in a laboratory where it is recorded as the pressure required to displace some wetting phase by a non-wetting phase to establish equilibrium.^[10] For reference, capillary pressures between air and brine (which is a significant system in the petrochemical industry) have been shown to range between 0.67 and 9.5 MPa.^[11] There are various ways to predict, measure, or calculate capillary pressure relationships in the oil and gas industry. These include the following:^[7]

The Leverett J-function serves to provide a relationship between the capillary pressure and the pore structure (see Leverett J-function).

This method is well suited to irregular rock samples (e.g. those found in drill cuttings) and is typically used to understand the relationship between capillary pressure and the porous structure of the sample.^[12] In this method, the pores of the sample rock are evacuated, followed by mercury filling the pores with increasing pressure. Meanwhile, the volume of mercury at each given pressure is recorded and given as a pore size distribution, or converted to relevant oil/gas data. One pitfall to this method is that it does not account for fluid-surface interactions. However, the entire process of injecting mercury and collecting data occurs rapidly in comparison to other methods.^[7]

The Porous Plate Method is an accurate way to understand capillary pressure relationships in fluid-air systems. In this process, a sample saturated with water is placed on a flat plate, also saturated with water, inside a gas chamber. Gas is injected at increasing pressures, thus displacing the water through the plate. The pressure of the gas represents the capillary pressure, and the amount of water ejected from the porous plate is correlated to the water saturation of the sample.^[7]

The centrifuge method relies on the following relationship between capillary pressure and gravity:^[7]

${\displaystyle p_{c}=hg(\rho _{w}-\rho _{nw})}$

where:

${\displaystyle h}$ is the height of the capillary rise

${\displaystyle g}$ is gravity

${\displaystyle \rho _{w}}$ is the density of the wetting phase

Zdroj:https://en.wikipedia.org?pojem=Capillary_pressure
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