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While the orthogonal components of the EM field were measured using the high-frequency EM method, the tensor measurements of the electrical and magnetic field components were used in the CSAMT method.
Three orthogonal components (N-S, E-W, and vertical) of the magnetic field were measured using three induction coils.
In this study, the soil-surface CO2 effluxes in an oasis cotton field were measured using the chamber method, and the CO2 concentrations were used to estimate the CO2 production in different layers of the soil profile using the gradient method.
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The Hall effect signal in a magnetic field is measured using this configuration, which also makes it possible to perform resistance measurements by the four-probe method.
The velocity field was measured using ordinary high-speed PIV.
The flow field was measured using the two-frame cross-correlation technique.
After loading, the strain field was measured using a moiré interferometer.
The temperature field was measured using 5 kHz chirped-probe-pulse (CPP) femtosecond (fs) coherent anti-Stokes Raman scattering (CARS).
Electrical current is applied through two outer electrodes, while the potential of the generated electrical field is measured using two inner electrodes.
The magnetic field is measured using a hall probe along the X, Y and Z axes from the centre of the pole pieces of the electromagnet.
The flow field is measured using particle image velocimetry (PIV), and the dominant unsteady vortex structures are determined using proper orthogonal decomposition.
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