One method to determine the resistivity structure of the earth, the magnetotelluric (MT) sounding method (Cagniard, 1953; Vozoff, 1972), is widely used especially for deep sounding. The surface impedance of the earth is measured for natural electromagnetic (EM) waves, and the apparent resistivity is calculated as a function of frequency. The MT sounding curve is a plot of the apparent resistivity with respect to the frequency. This representation of the sounding curve at larger abscissa (higher frequency) shows the shallower structure. Sometimes the sounding curve is plotted with respect to the period (the inverse of the frequency), so that the larger abscissa (longer period) corresponds to the deeper structure, as is the case for the Schlumberger sounding curve.