3.1. Soil matric suction measurement Matric suction is the difference between the pore-air and pore-water pressures within
the unsaturated soil structure. Matric suction measurement can be done through direct
and indirect measurements. In the direct measurement method, only the negative
pore-water pressure is measured as the pore-water pressure is usually equal to the
atmospheric pressure. A Tensiometer is the most commonly used device for direct
measurement of negative pore-water pressure in the field. It consists of a high-air-entry
(HAE) porous ceramic cup that is attached to a pressure gauge with a small plastic tube,
filled with de-aired water. Once the HAE ceramic cup is in contact with the soil
particles and the equilibrium is reached, the water in the tube will have the same
negative pressure as the soil pore-water pressure that can be read using the device
pressure gauge. This measurement is numerically equal to the matric suction if the
pore-air pressure is equal to the atmospheric pressure. The indirect measurement of the
matric suction is done by measuring a different variable than the negative pore-water
pressure.
In indirect measurement methods, the electrical or thermal conductivity of a porous
material, which is a function of its moisture content, is measured. Since water content is
also a function of the matric suction, the matric suction of the sensor and the
surrounding soil can be determined using predefined calibration curves (Fredlund et al.,
2012).
3.2. Axis translation technique The negative pore-water pressure that can be directly measured with a tensiometer is
limited to about -1 atm. (~-100 kPa) as there is the risk that the water in the tensiometer
may begin to cavitate and interfere the measurements. In order to measure matric
suctions over this range, the axis translation technique is usually employed in the
laboratory. In this technique, the soil specimen is exposed to a certain air pressure in a
closed chamber, and therefore the origin of the pore-water pressure is translated from
the standard atmospheric pressure to the air pressure of the chamber. Thus, the risk of
cavitation is avoided as the pore-water pressure does not go below -1 atm. In other
words, both the pore-air and pore-water pressures are translated, while the matric
suction (
w a u u
) in the specimen is maintained (Hilf, 1959; Fredlund, 1989).