Timing delays between data acquisition and gradient transmission result in image degradation. This is especially true in spiral MRI, where delays can alter data in a nonuniform manner, generating significant artifact in the reconstructed data. The many methods that exist to mitigate these delays or measure the k-space coordinates require long measurement times, complicated analysis, specialized phantoms or hardware, or significant changes to the sequence of interest. A fast and simple method is proposed to measure delays on each gradient channel. It requires only minimal modification to an existing spiral sequence and can be used to measure independent delays on three gradient channels and any scan subject within six sequence repetition times. Accurate reconstruction of MRI data requires knowledge of the k-space sample locations. Deviations from the theoretical gradient waveforms can be caused by eddy currents, gradient amplifier nonlinearities, and other system imperfections. These deviations take the form of gradient timing delays and amplitude distortions that result in altered sample locations in k-space, producing artifacts in the reconstructed images. In spiral trajectories, these artifacts can be mistaken for aliasing, loss of resolution, poor signalto noise-ratio, or off-resonance blurring, thus making the source of the artifacts difficult to discern.Modern MRI scanners mitigate eddy currents through the use of gradient coil shielding and gradient waveform preemphasis. Sequences that place large gradient slew-rate and amplitude demands on the hardware can induce eddy currents, despite gradient coil shielding. Gradient waveform pre-emphasis provides an additional level of eddy current compensation but can only be optimized for a limited range of sequences. A number of techniques have been employed to compensate for the remaining deviations from the expected k-space coordinates.Several strategies seek to measure the actual gradient waveform for correct reconstruction or improved gradient pre-emphasis. Spielman and Pauly (1) directly measured the current on each gradient channel. Errors from the gradient amplifier were directly measured, but eddy currents were assumed to be negligible. Onodera et al. (2) proposed