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From our synthesis model, the body resonator has a driving-point admittance that filters the output of the string model to transform force waves along the string into acceleration waves at the bridge [44]. Taking the inverse-FFT of the measured driving-point admittance, we obtain the impulse response of the body of the instrument. This time-domain signal can be stored as a wavetable for convolution with the output of the synthesis string-model. Figures 39, 40, 41 and 42 show the time-domain signal and spectrum (both magnitude and phase) of a measured guitar's body impulse response, respectively. As shown, the impulse response lasts well over ms long. Viewing its spectrum in Figure 41, we note peaks that occur near and Hz.