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In laboratory car crash tests, Anthropomorphic Test Devices (ATD) are equipped with piezoresistive and resistive sensors for occupant injury assessment. Accelerometers are inertial transducers that convert acceleration into electrical output which can be easily recorded by a Data Acquisition System (DAS). For an accelerometer, this electrical output mainly depends upon subjected acceleration, sensitivity of the accelerometer, excitation voltage and gain provided. Before use in testing, accelerometers are calibrated at a standard excitation (manufacturer decided) voltage to determine characteristics like Sensitivity, Sensitivity per unit excitation voltage, Zero Measurand Output (ZMO), Transverse Sensitivity etc. It is observed that these characteristics are highly dependent on the excitation voltage. In testing, due to limitations of DAS and/or other unwanted noise in the excitation voltage, these accelerometers are sometimes used at a different excitation voltage.

This article brings a practical analysis for determination of gravity center in unsymmetrical three dimensional bodies practically and graphically. The gravitational center of an object is the point from which if suspended, the object remains stable at all times, this is also called as center of mass of the object, or the theoretical point at which the entire weight of the object is assumed to be concentrated. In certain tests, the Center of Gravity (CG) of the Seat is required to be known, for load application. The CG is the point at which a SEAT would balance if it were possible to suspend it at that point. This paper deals with use of applied engineering and theoretical calculations to ascertain the CG of First and Second Row seats (individual and bench type). In this case the center of gravity location is expressed in units of length along each of three axes (X, Y and Z). Load balance equation is used to calculate the CG of the seat.