elkcub
Silicon Valley, California
Hi Ron,
I'm about played out on this, but I do remembered your method for measuring rotation angles. Unfortunately, it's very difficult for me to tape a paper scale around focusing wheels. So I use markings on the wheel itself and measure rotation against a fixed reference point on the body. The 8x42 HD's wheel, for example, has 36 ridges, each representing 360/36 = 10˚ rotation. The 10x42 SLC and 7x42 Zeiss have 16 equally spaced diopter marks, each representing 22.5˚ rotation. Interpolation may be effective to ±10˚, but DOF variations are by far the biggest obstacle, and would require impractical procedural controls.
I like your idea for a mini torque meter, although some binoculars would be much more difficult to instrument than others. The 7x42 BGAT*P, for example, has a very narrow wheel. If that could be overcome, though, string length might also be a neat way to measure rotation angles, given a known wheel radius.
My primary interest is erg-o-nomics (literally, "work" measurement), so I directed this analysis at the push/pull efforts required for changing working distances. There have been various assertions about the 8x42 SLC HD being too slow, i.e., that more effort is required than with "normal" or older instruments. However, putting Kimmo's results together with mine, I'm satisfied that the SLC HD simply has a greater focusing range, which increases the number of push/pulls and perhaps gives the false impression that it's slower. Between 10m and infinity, at least, these three birding binoculars behaved about the same. Curiously, the simplified 8x42 SLC design appears to be significantly slower, so I'm wondering how economy can be realized when basic performance is compromised.
Ed
I'm about played out on this, but I do remembered your method for measuring rotation angles. Unfortunately, it's very difficult for me to tape a paper scale around focusing wheels. So I use markings on the wheel itself and measure rotation against a fixed reference point on the body. The 8x42 HD's wheel, for example, has 36 ridges, each representing 360/36 = 10˚ rotation. The 10x42 SLC and 7x42 Zeiss have 16 equally spaced diopter marks, each representing 22.5˚ rotation. Interpolation may be effective to ±10˚, but DOF variations are by far the biggest obstacle, and would require impractical procedural controls.
I like your idea for a mini torque meter, although some binoculars would be much more difficult to instrument than others. The 7x42 BGAT*P, for example, has a very narrow wheel. If that could be overcome, though, string length might also be a neat way to measure rotation angles, given a known wheel radius.
My primary interest is erg-o-nomics (literally, "work" measurement), so I directed this analysis at the push/pull efforts required for changing working distances. There have been various assertions about the 8x42 SLC HD being too slow, i.e., that more effort is required than with "normal" or older instruments. However, putting Kimmo's results together with mine, I'm satisfied that the SLC HD simply has a greater focusing range, which increases the number of push/pulls and perhaps gives the false impression that it's slower. Between 10m and infinity, at least, these three birding binoculars behaved about the same. Curiously, the simplified 8x42 SLC design appears to be significantly slower, so I'm wondering how economy can be realized when basic performance is compromised.
Ed
Last edited: