Pressure potential (\(Psi_p\)) is the physical pressure exerted on a fluid within a confined space, fundamental to the movement and support of water in plants. It represents the hydrostatic pressure, or the force per unit area, that water molecules exert on the cell boundaries. This physical force can be either positive (pushing outward) or negative (pulling inward). The magnitude and direction of this pressure determine the energy state of water and are central to processes like maintaining plant structure and long-distance water transport.
Context: Pressure Potential as Part of Water Potential
Pressure potential is one of the components that define the total water potential (\(Psi\)), which is the measure of the potential energy of water in a system relative to pure water. Water potential predicts the direction of water movement, as water always moves from an area of higher potential (less negative) to an area of lower potential (more negative). The comprehensive formula for water potential is \(Psi = Psi_s + Psi_p + Psi_g + Psi_m\), where each term is a form of potential energy.
The pressure potential (\(Psi_p\)) is summed with the solute potential (\(Psi_s\)) and the gravitational potential (\(Psi_g\)). Solute potential accounts for dissolved substances, which reduce the free energy of water, making \(Psi_s\) negative or zero. Gravitational potential (\(Psi_g\)) accounts for the influence of gravity, but its effect is often considered negligible in smaller plants. The matric potential (\(Psi_m\)), which accounts for water adhesion to surfaces, is also usually ignored in fully hydrated plant cells.
For most physiological calculations in plant tissues, the simplified equation \(Psi = Psi_s + Psi_p\) is used, emphasizing the interplay between solute concentration and physical pressure. The standard unit for expressing all forms of water potential is the Megapascal (MPa). This unit is used because the components represent energy per unit volume, which is dimensionally equivalent to pressure.
Positive Pressure: The Role of Turgor
When water moves into a plant cell, it creates a positive pressure potential known as turgor pressure, which is the most recognizable function of \(Psi_p\). This positive pressure arises from osmosis, where water flows into the cell’s central vacuole due to a lower solute potential inside the cell compared to the exterior. As the vacuole fills, it expands and pushes the flexible plasma membrane outward against the rigid cell wall.
The cell wall’s structural integrity resists this expansion, generating an equal and opposite inward force, which is the measurable turgor pressure. This hydrostatic pressure makes non-woody plants rigid, allowing them to remain erect against gravity; well-watered plants can have turgor pressures of \(0.6\) to \(0.8\) MPa. When a plant loses water, turgor pressure drops, leading to wilting as the cells lose structural support.
Turgor pressure also drives cell expansion during growth, as the outward force on the cell wall loosens its structure, allowing the cell to enlarge. Specialized cells, such as the guard cells surrounding the stomata, use regulated changes in turgor pressure to control gas exchange. When water flows into the guard cells, increased turgor causes them to swell and bow outward, opening the stomatal pore for carbon dioxide uptake. Conversely, a decrease in turgor causes the guard cells to become flaccid and close the pore to conserve water.
Negative Pressure: Driving Water Through the Xylem
In the plant’s vascular tissue, the xylem, pressure potential shifts from a positive pushing force to a negative pulling force, or tension. This tension is the primary force responsible for transporting water and dissolved minerals from the roots to the furthest leaves, often against the force of gravity. The water column in the xylem is under negative pressure potential, which can reach values as low as \(-2\) MPa at the leaf surface of a transpiring plant.
This upward pull is explained by the Cohesion-Tension theory, which posits that the evaporation of water vapor from the leaves, known as transpiration, is the engine of water movement. As water evaporates through the stomata, it creates a strong negative pressure in the leaf’s mesophyll cells, which is transmitted down to the continuous column of water in the xylem.
The cohesive properties of water molecules, which stick to one another through hydrogen bonds, allow the entire column to be pulled upward like a single, unbroken rope. Adhesive forces between water molecules and the hydrophilic walls of the narrow xylem vessels also assist in maintaining this continuous water column. However, the integrity of this column can be compromised if the tension becomes too great or if air enters the system, leading to cavitation. When an air bubble forms, the continuous water pathway is broken, effectively blocking the flow of water.

