The theoretical concept of distributed acoustic sensing (DAS) is based on the principle that scatters in the glass fibers are frozen in place when the cable is manufactured. When the cable is utilized as part of a DAS field-system, the motion of the ground compresses and elongates with the buried cable causing differences in the travel-time from laser pulses which are back scattered to the interrogator. This use of reflectometry to measure the change in position between scatters for strain rate is key in measuring the true ground deformations. However, the relation between strain rate and particle motions is not well understood nor frequently demonstrated experimentally in the field when DAS is compared with traditional three-component (3C) particle motions. This is particularly true as to the variability due to spatial distance scales and frequency ranges at which surface axial strain rate, areal strains, and particle motions are comparable.Previous studies have tried to quantify the distance range and frequencies at which local strain at the surface are comparable to strain approximated by particle motions using seismic arrays. For example, Gomberg et al. (1999) performed a similar analysis comparing array derived strains with point estimates from seismometers for two frequency bands, 0.5-1 and 4-8 Hz. They found agreement in dynamic strains at 0.5-1 Hz; however, at higher