PTU-treated 2 to 4 dpf zebrafish were euthanized and lens transparency assessed using a microscope (Zeiss Axioplan 2; Oberkochen, Germany) with differential interference contrast (DIC) optics, which highlighted refractive abnormalities. Images were captured using a digital camera (ORCA-ER; Hamamatsu Photonics KK, Hamamatsu City, Japan) and acquired using commercial software (Velocity 5, version 5.2.1; PerkinElmer, Akron, OH, USA). Larval or adult zebrafish were euthanized and transparency of dissected lenses was visualized with a microscope and digital camera with a dynamic positioning controller (Olympus SZX12 microscope and Olympus DP70 with a model 2.1.1.183 controller; Olympus Corp., Tokyo, Japan). For in situ transparency assessment, a fiber optic light source (Schott KL 1500; Schott AG, Mainz, Germany) was used for oblique illumination from two sides to visualize opacities. Standard length and eye diameter were measured following previously established guidelines.
30 Lenses were dissected in phosphate buffered saline (PBS) (Fisher BioReagents, Pittsburgh, PA, USA) at room temperature (RT) and images were used to assess transparency under darkfield and brightfield illumination. Optical properties were assessed by the ability of lenses to focus a field finder grid (Lovins Field Finder; Electron Microscopy Sciences, Hatfield, PA, USA). Lenses were oriented equatorially, with poles and sutures perpendicular to the plane of focus, or axially, with poles and sutures parallel to the plane of focus. Zebrafish lenses are not completely rotationally symmetrical, so to determine lens size, diameters were measured in an equatorial orientation. The position of the lens nucleus center was normalized to lens size by expressing the position of the nucleus as the normalized coordinate,
r/
a, where
a is the radius of the lens and
r is the distance from the center of the lens to the center of the nucleus. The value of (
a − r) is the distance of the center of the nucleus from the anterior pole, which is the number we actually measured, since it is difficult to precisely locate the center of the lens. We calculated the value of
r/
a as [1 − (
a −
r)/
a], where
a and (
a −
r) were the actual measured values, for experimental convenience. For a nucleus at the center of the lens (
r = 0), the value of the normalized coordinate
r/
a is 0. For a nucleus centered at the surface of the lens (possible only for a point nucleus) the value of the normalized coordinate
r/
a is 1. In fact, we never observed a nucleus center closer to the surface than an
r/
a value of about 0.5.
r/
a was graphed as a function of standard length (SL). The positions of centers of adult nuclei were measured when the presumptive embryonic nucleus was evident.