Notes on Voyager Quick Look Data: Since Oct 2, 2006, "quick-look" magnetic field data for Voyagers 1 & 2 have been posted on the Internet within a day or two of acquisition by the spacecraft. The rapid availabililty is achieved at the expense of the quality of the data. The quick-look data are processed with the last available roll and zero level data. The quick-look data are very preliminary and must be used with the greatest caution. At the time of experiment proposal, the mission (then called "Mariner-Jupiter/Saturn") was designed to investigate Jupiter, Saturn and the interplanetary medium out to Saturn at 10 AU, where the interplanetary magnetic field strength is 0.6 nT. These objectives determined the required accuracy of the measurements, which together with the nature of the spacecraft determined the design of the instrument. The spacecraft magnetic field at the outboard magnetic field sensor, referred to as the primary unit, was expected to be 0.2 nT and highly variable, consistent with current estimates. Hence, the dual magnetometer design (Ness et al., 1971; Behannon et al. 1977). At distances > 80 AU, the magnetic field strength is less than ~0.05 nT in the solar wind, an order of magnitude smaller than the instrument was designed to measure and a fraction of the spacecraft magnetic field strength at the outboard sensor. Thus physical signal measured by the Voyagers is a fraction of the highly variable non-Gaussian noise that produced primarily by the spacecraft. The use of roll calibrations lasting ~6 hours permits determination of the effective zero levels for the two independent magnetic axes that are perpendicular to the roll axis (which is nearly parallel to the radius vector to the Sun) at intervals of ~ 3 - 4 months. Two successive rolls are required to extract the signal from the noise. There is no roll calibration for the third magnetic axis; data for a month after an additional month after a roll are required to calibrate the third axis. Data between two successive rolls + 1 month are required in order to extract the signal from the noise. Given this information, a comparison of the two derived magnetic vectors from the two magnetometers permits validation of the primary magnetometer data with an accuracy of 0.015 nT - 0.05 nT. A discussion of the uncertainties that must be considered when using the fully processed data is given in the Appendix of Burlaga et al. [1994] and in Appendix A of Burlaga et al. [2002]. Since the quick look data are necessarily processed with information from only one (the last) roll, the information required to extract the signal from the noise is not available after that roll, and the uncertainties in the quick-look data can be very large. Indeed, in general, the quick-look data are dominated by the variable spacecraft magnetic field.