The aim of this study was to adapt the balloon model for BOLDbased MR signal changes to a magnetic field strength of 3T and to examine its validity. The simultaneous measurement of BOLD and diffusion-weighted BOLD responses was performed. The amplitude of the BOLD peak was found to be similar for all subjects when a short visual stimulus of 6 sec was used. The rise-time to the BOLD peak and the shape and depth of the poststimulus undershoot varied significantly. A fit of the experimental BOLD responses was found to be possible by use of parameters within a reasonable physiological range. The relations between these parameters and their influence on the modeled BOLD responses is discussed. A prediction of the balloon model is the occurrence of a BOLD overshoot, i.e., a lag between the changes of the blood volume and the blood flow after the start of the stimulation. Functional MRI is based on measuring the local changes in the blood oxygenation level dependent (BOLD) contrast that occur as a consequence of neuronal activation in the brain (1-3). The change in the MR signal is determined by alterations in the concentration of paramagnetic deoxyhemoglobin, which modifies the effective transverse relaxation time T* 2 . Increases in oxygen consumption and blood volume lead to an increase in the deoxyhemoglobin content and hence to a decreased MR signal, whereas increases in blood flow have the opposite effect (4). Although considerable progress has been made in measuring the changes in oxygen consumption (5-7), blood volume (8,9), and cerebral blood flow (6,10,11), the transient response in the BOLD signal is still not completely understood. It can be divided into three intervals: the fast response (12-15), during which the signal change is negative, the period of elevated signal, and the poststimulus undershoot (3). In order to understand the origins of these signal changes it is desirable to relate the BOLD signal directly to the relevant physiological parameters.The most prominent approach developed to date for modeling the BOLD signal under nonsteady-state conditions is given by the balloon model of Buxton et al. (10). Based on the experimental work of Mandeville et al. (8), who showed that changes in blood volume occur subsequent to changes in blood flow, it considers the vasculature contributing to the BOLD signal as a swelling balloon. The basis of the model is a differential equation system for the blood volume and the total deoxyhemoglobin content, combined with an expression for the total signal change. The results of simulations for the intra-and extravascular signal contributions (16,17) and the oxygen limitation model (18) were used in order to derive time courses for the BOLD signal response.In order to study the time courses of the deoxyhemoglobin concentration and the blood volume in detail it is advantageous if the contributions of the intra-and extravascular spaces can be evaluated separately. This may be achieved by using a weak diffusion weighting to suppress the signal from the intravascular comp...