The time-harmonic solution for the anomnalous vector potential due to a conducting permeable sphere in the field of a currentcarrying loop is used to derive the corresponding step response. The step response is then used to obtain analytical expressions for the voltage induced in a second loop due to a chosen exciting current pulse train. The voltage induced in an actual system of coils is obtained by superposition. The effect of the measurement system is included in the analysis in order to experimentally verify the model. Measured responses of a number of aluminum and steel spheres at various distances from the coils are compared with theoretical predictions. The agreement between the two is generally good. I. INTRODUCTION THE USE OF electromagnetic induction in detecting conducting objects is well established in geophysics [1], nondestructive testing [2], [3], treasure hunting [4], and mine detection [5], among other disciplines. A conducting object is exposed to a time-varying (usually in the hertz to kilohertz range) magnetic field produced by a current-carrying primary coil. The resulting eddy currents in the object produce a secondary magnetic field, which is detected by another coil. A particular choice of time variation of the primary current and the number and relative positions of coils is dictated by operational considerations and ease of data interpretation in a given application. The work reported here is directed towards detectors of buried artillery shells, which are small (diameters -0.02-0.15 m, lengths -0.05-0.70 m, masses -0.1-45 kg), metallic (a-107 S/m) objects at shallow depths (0-2 m). For this application, a pulse train of primary current and a vertical coaxial sensor geometry, as shown in Fig. 1, are considered most suitable [6], [7]. Detectors of this type are commercially available and simplified analysis of signals induced in them by metallic objects are reported [8]. However, detailed analysis taking into account the effects of pulse shape, finite coil size, and measurement system parameters is not available. This paper presents such an analysis for a metallic sphere. This would provide a useful model for predicting detector performance and for possible processing of measured signals to extract information about a detected object such as its depth, size, or material properties.