Votre auditoire peut devenir le meilleur ambassadeur de votre projet : à vous de le persuader. En s'appuyant sur une analyse attentive des discours des plus grands orateurs, Nancy Duarte vous aide à faire de vos présentations de véritables aventures visuelles. Comme l'écrit Nancy Duarte dans son introduction, « ce livre sert simultanément de guide, de manuel et de défense du storytelling comme méthode de communication dans le monde des affaires. Il vous permettra d'atteindre un niveau de présentation que peu de gens dominent. Grâce à des techniques issues de l'art narratif et du cinéma, vous maîtriserez les étapes essentielles pour toucher votre public, vous tenir en retrait pour l'élever au rang de héros de l'histoire et créer une présentation qui résonne.»
Explores how all vibrations are essentially the one spirit in motion.
1.6 A ball of mass m fits snugly ( but with negligible friction ) inside the neck of a bottle ( see figure ) . The neck has cross - sectional Jol area A ; at equilibrium , the volume of the bottle below the ball is V and is filled with ...
This introductory text emphasises physical principles, rather than the mathematics.
Just Vibrations: The Purpose of Sounding Good calls for a time-out in our serious games of critical exchange.
Vibrations and Waves in Continuous Mechanical Systems provides a first course on the vibrations of continuous systems that will be suitable for students of continuous system dynamics, at senior undergraduate and graduate levels, in ...
Lucid and beyond traditional writing style makes the text different from other books. In this text, every effort has been taken to make the subject easy and interesting.
Mechanical Vibrations
This book is intended for engineers who deal with vibrations of rods and shells in their everyday practice but also wish to understand the subject from the mathematical point-of-view.
This book studies methods for a robust design of rotors against self-excited vibrations.
Theory and Practice Paul H. Wirsching, Thomas L. Paez, Keith Ortiz. Let W have a mean of zero and let it be ... If the “signal” aX is twice as strong as the noise, then r = % and PXY = 0.9; the dependence is considered strong.