The experiments showed that the SLEA tilts exhibited significantly more detail for radar echoes, particularly those comprised of vertically shallow precipitation, at farther distances from the radar site. This was expected as the SLEA tilt remains closer to the terrain surface hence the sample beam volume does not overshoot as much of the precipitation bearing clouds than the 0.5° tilt. It was also noted that a dual pol vertical profile of reflectivity correction (dpVPR) was sometimes not attempted for SLEA tilts, hence bright band contaminated reflectivity data would negatively impact QPE. Subsequent investigation revealed that the melting layer top pattern in the RhoHV field extended to near the maximum distance of dual pol data in these instances. Hence, the dpVPR algorithm could not determine a full melting layer structure, including the top, and therefore did not make a bright band correction to reflectivity within the melting layer. Further, the melting layer bottom signature in the RhoHV field appears less significant in the SLEA tilt than in the 0.5° tilt due to the associated larger sample beam volumes at farther distances. This impact sometimes caused the melting layer bottom to be diagnosed further from the radar than it should be, resulting in a wet bias in specific attenuation derived QPE due to contamination from frozen hydrometeors.

