I work at the Department of Astronomy, University of Baghdad. I do research in Observational Astronomy, Astrophysics and Astronomy, optics and Image processing. I graduated from Florida Institute of Technology in 2015 with a Ph.D. in physics. My most recent publications are "Painterly Rendering by Using K-mean Segmentation" and "Designing Cassegrain Telescope System with the Best Obscuration Ratio of Secondary Mirror".
Ph.D. in Physics Msc. in Physics Bsc. in Astronomy and Space
Image processing / Optics/ Modeling/ Astronomy/ Astrophysics
Photometry Image Processing Observational Astronomy Astrophysics Optics Computational Physics
Mathematical Modeling
The problem statement discussed in this paper is a new technique for the presentation of painterly rendering that uses a K-mean segmentation to divide the input image into a set of regions (depending on the grayscale of the regions). Segmenting the input image helps users use different brush strokes and easily change the strokes' shape, size, or orientation for different regions. Every region is painted using different brush kinds. The properties of the brush strokes are chosen depending on the region's details. The brush stroke properties, such as size, color, shape, location, and orientation, are extracted from the source image using statistical tools. The number of regions is set up manually and depends on the input image. This
... Show MoreA computer simulation was conducted using Optics Software for Layout and Optimization (OSLO) to design a Cassegrain telescope system for on-axis rays. In order to establish such a telescope, the two mirrors of the optical system were designed as spherical surfaces: a concave mirror and a convex mirror. The obscuration ratios of the Cassegrain telescope's secondary mirror were examined using different values, which ranged between 0.1 and 0.3, to determine the best obscuration ratio. This work adopted three criteria to decide which obscuration ratio is the best for the Cassegrain telescope. The first criterion was the number of rays that reached the final image. The second criterion was calculating the modulation transfer function
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