Search results with tag "Lecture 17"
Three-Dimensional Coordinate Systems
www.math.usm.eduJim Lambers MAT 169 Fall Semester 2009-10 Lecture 17 Notes These notes correspond to Section 10.1 in the text. Three-Dimensional Coordinate Systems
6Microfluidics Theory handouts - University of California ...
www-bsac.eecs.berkeley.edu1 EE C245 Picture credit: Sandia National Lab Fluidic Dynamics Dr. Thara Srinivasan Lecture 17 Picture credit: A. Stroock et al., Microfluidic mixing on a chip
Lecture 17 - School of Physics and Astronomy
www2.ph.ed.ac.ukcan be projected using P onto the space spun by the degenerate states: P Vˆ −E 1 ψ 0 =0. (17.25) Choosing a basis for the space of degenerate levels, we can write ψ 0 as: ψ 0 = g0 i=1 c i φ i, (17.26) and then rewrite Eq. (17.25): φ i|Vˆ|φ jc j = E 1 c i, (17.27) i.e. E 1 is an eigenvalue of the matrix V ij = φ i ...
Lecture 17: Huffman Coding
home.cse.ust.hkquencies. Then is an optimal code tree in which these two letters are sibling leaves in the tree in the lowest level. Proof: Let T be an optimum prefix code tree, and let b and c be two siblings at the maximum depth of the tree (must exist because …