Daniel bernoulli economics
- 10 interesting facts about daniel bernoulli
- Daniel bernoulli contributions to mathematics
- Daniel bernoulli atomic theory
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Bernoulli's principle
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Daniel Bernoulli
Daniel Bernoulli (8 de febreru de 1700, Groningen – 17 de marzu de 1782, Basilea) foi un matemáticu, estadísticu, físicu y médicuholandés-suizu. Destacó non yá en matemática pura, sinón tamién nes llamaes aplicaes, principalmente estadística y probabilidá. Fixo importantes contribuciones en hidrodinámica y elasticidá.
Vida
[editar | editar la fonte]Daniel Bernoulli provenía de la saga familiar de Bernoulli, que xeneró grandes meyores matemátiques a lo llargo de la historia. Yera fíu de Johann Bernoulli y nació en Groningen, Países Baxos, onde'l so padre yera entós profesor de matemátiques. En 1705, el so padre llogra una plaza na Universidá de Basilea y la familia torna a la ciudá suiza d'onde yera orixinaria.
Por deséu del so padre estudió Medicina na Universidá de Basilea, ente qu'al empar, na so casa, el so hermanu mayor Nicolau y el so padre ampliaben les sos conocencies matemátiques. Daniel remató los estudios de Medicina en 1721. En principiu intentó entrar como profesor na Universidá de Basilea,
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Hydrodynamica
Book by Daniel Bernoulli
Hydrodynamica (Latin for Hydrodynamics) is a book published by Daniel Bernoulli in 1738.[1][2] The title of this book eventually christened the field of fluid mechanics as hydrodynamics.
Contents
The book deals with fluid mechanics and is organized around the idea of conservation of energy, as received from Christiaan Huygens's formulation of this principle. The book describes the theory of water flowing through a tube and of water flowing from a hole in a container. In doing so, Bernoulli explained the nature of hydrodynamic pressure and discovered the role of loss of vis viva in fluid flow, which would later be known as the Bernoulli principle. The book also discusses hydraulic machines and introduces the notion of work and efficiency of a machine. In the tenth chapter, Bernoulli discussed the first model of the kinetic theory of gases. Assuming that heat increases the velocity of the gas particles, he demonstrated that the pressure of air is proportional to kinetic energy of gas particles, thus
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