Time resolved laser induced incandescence (LII) technique is used to measure size distribution of soot nanoparticles of candle's flame. Pulsed Nd:YAG laser is used to heat nanoparticles to incandescence temperature and the resulting signal is measured. Mass and energy balance equations are numerically solved to calculate temperature of soot particles in low fluence regime. Assuming Plank black ...

Background. Force production and movement in sports are predominantly performed in a unilateral weight-bearing stance, therefore a resistance training program should closely resemble sport specific unilateral leg kinetics. Hipand trunk-stabilizing muscle activity increases as the relative body weight balance changes from a bilateral to a unilateral stance, and these muscles are thought to play ...

form (R. A. Paulsen, S. Fujita, S. C. Smart, and D. F. Stowe. FASEB J. 11: A526, 1997). Present address of S. Fujita: Dept. of Anesthesiology, Minami 1-Jyo Hospital, S-1, W-13, Chuo-ku, Sapporo Medical University, Hokkaido 060, Japan. Address for reprint requests and other correspondence: D. F. Stowe, M4280 MEB, 8701 Watertown Plank Rd., Medical College of Wisconsin, Milwaukee Regional Medical ...

7 Matthew R. Hodges and George B. Richerson 8 9 Dept of Physiology, Medical College of Wisconsin, Milwaukee, WI 53226 10 11 Departments of Neurology and Cellular and Molecular Physiology, 12 Yale University, New Haven, CT 06520 13 14 Veteran’s Affairs Medical Center, West Haven, CT 06516 15 16 Address for Correspondence: 17 Matthew R. Hodges 18 BSB-504, Dept of Physiology 19 Medical College of ...

Aaron B. Wong ( ),1,3,4 Zhizi Jing ( ),1,2,3,4 Mark A. Rutherford,1 Thomas Frank,1 Nicola Strenzke,1,2,3 and Tobias Moser1,3,5,6 1InnerEarLab, 2Auditory Systems Physiology Group, Department of Otolaryngology, and 3Collaborative Research Center 889, University Medical Center Göttingen, D-37099 Göttingen, Germany, 4International Max Plank Research School for Neuroscience, Göttingen Graduate Schoo...

J. Hoppler,1,2,* J. Stahn,2 H. Bouyanfif,1,† V. K. Malik,1 B. D. Patterson,3 P. R. Willmott,3 G. Cristiani,4 H.-U. Habermeier,4 and C. Bernhard1 1Department of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Chemin du Musée 3, CH-1700 Fribourg, Switzerland 2Laboratory for Neutron Scattering, ETH Zurich & Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland 3Swiss Lig...

1Vascular Biology and Therapeutics Program, Yale University School of Medicine, New Haven, Connecticut, USA; 2Integrative Cell Signaling and Neurobiology of Metabolism Program, Section of Comparative Medicine and Department of Pathology, Yale University School of Medicine, New Haven, Connecticut, USA; 3Departments of Medicine, Leon H. Charney Division of Cardiology, and Cell Biology, New York U...

Let F be a non-zero polynomial with integer coefficients in N variables of degree M . We prove the existence of an integral point of small height at which F does not vanish. Our basic bound depends on N and M only. We separately investigate the case when F is decomposable into a product of linear forms, and provide a more sophisticated bound. We also relate this problem to a certain extension o...

The Poincaré–Hardy inequality ∫ |u| dist(x,E) dm ≤ K · ∫ | u |dm is derived in R3 on the complement of a Cantor set E. We use a special self-similar tiling and a natural metric on the space of trajectories generated by a Mauldin–Williams graph which is homeomorphic with the space of tiles endowed with the Euclidean distance. A crude estimation of the constant K is 2,100. Two applications will b...