РефератыИностранный языкBeBernoullian Thoughts Essay Research Paper Daniel Bernoulli

Bernoullian Thoughts Essay Research Paper Daniel Bernoulli

Bernoullian Thoughts Essay, Research Paper


Daniel Bernoulli was born into a family of


mathemeticians on February 8, 1700. He was the only person


in his family to make an impressive mark on physics.


Bernoulli became a Swiss physicist and mathmatician who made


enourmous contributions to the world of physics. He


uncovered many significant phenomena in hydrodynamics, and


in 1738, published his most famous work, Hydrodynamica,


which was a study of equilibrium, pressure, and velocity of


fluids. He proved that as the velocity of fluid flow


increases, its pressure decreases. Bernoulli?s principle


was an early formulation of the subsequent idea of ?the


conservation of energy?.


Bernoulli?s Hydrodynamica was also the first attemt to


explainof the behavior of gasses with changing pressure and


temperature. This was the beginning of the kinetic theory of


gasses. His gas model has been revived and transformed into


a powerful theory regarding the thermal and mechanical


properties of gases using the atomic hypothesis.


Bernoulli thought of the ?corpuscles? of the gas as so


minute that there were ?practically an infinite number?


under ordinary conditions, even in a small container. In


their rapid motion, these corpuscles collide with each other


and also with the rigid walls of the closed vessel. The


collisions, however, can be assumed to be perfectly elastic;


therefore, the kinetic energy of the particles is conserved


and the motion can continue undiminished. Therefore, the


pressure which the gas is expected to exert against all


sides of the container is caused by the incessant impact of


millions of high speed particles; hence the name ?impact


theory? of gas pressure.


Imagine a gas filled cylindrical container with the top


end that is able to slide up and down, in and out like a


piston. If the volume is slowly decreased, the corpuscles


are more crowded in the progressively smaller space and the


number of collisions per second with the walls would be


larger (i.e., the pressure should become greater, as


observed). Bernoulli even calculated the magnitude of this


expected increase and found that it corresponded to Boyle?s


experimental law.


At the time of Bernoulli?s discovery, his work was


generally ignored. The lack of general attention was due to


the unclear knowledge of gases. Yet more than a century


later, his work simultaneously clarified the main problems


of the nature of gases, heat and chemistry. For Bernoulli,


in effect, had made two enormous leaps in his thinking for


which most scientists were not ready to take. First, he


illucidates, the direct equivalence of heat and internal


molecular motion, ignoring any interactions between the two.


Second, he confirmed the idea that a well-defined numerical


relationship, such as Boyle?s simple law, could be deduced


from a chaotic picture of randomly moving particles.


Bernoulli?s principle was centerd around the notion


that we suppose a small portion of liquid flow from one


point to another point, and that change of position is


affected without incurring any waste of energy. From the


principle of conservation of energy, it may be asserted that


the total energy is not changed during the displacement.


This statement is known as Bernoulli?s theorem and is often


expressed as:


P + 1/2 pv2 + pgy = constant


Bernoulli?s equation states that the sum of the pressure


(P), the kinetic energy per volume (1/2 pv2), and the


potential energy per unit volume (pgy) have the same value


at all points along a streamline. Using Bernoulli?s law,


because there is no waste of energy du

ring the passage of


the liquid, the total energies at each three places are


equal. If the fluid is incompressible then the internal


energy is the same, which proves, in turn, that Bernoulli?s


equation holds true along any streamline.


Bernoulli?s foregoing principle explains a number of


phenomena about the behavior of liquids which, at first,


seem strange. Suppose two ships are steaming side by side


in still water: The relative motion of the ships with


respect to the water will remain unchanged if the ships are


imagined to be stationary and the water imagined to flow


with the same velocity in the opposite direction. the water


entrapped between the ships will speed up because of the


narrow space. As a consequence, the pressure in the water


between the ships will be reduced and will become less than


the water pressure on the far sides of the ships. The


excess pressure will cause the ships to become closer in


proximity.


Bernoulli?s theorem, when applied to gasses instead of


liquids, explains such effects as the curved flight of a


tennis ball that is spinning when served, the action of an


atomizer in dividing a jet of liquid into a fine spray, the


reduction of gas pressure in a container by using an


aspirator connected to a water faucet and the propulsion of


a ship by wind power using cylindrical rotors instead of


sails.


Bernoulli?s theorem provides a means for measuring the


flow of a liquid through a pipe. A section of pipe


containing a constriction or throat is inserted in the pipe


line and the pressures are measured both at the throat and


in the pipe by pressure gauges or their equivalent. The


rise of liquid in small tubes, called manometers, indicate


the pressure. The pipe beyond the throat flares out slowly


so that the velocity of the liquid can be reduced without


disturbing the streamline flow.


Since the velocity of the liquid is greater at the


throat than in the pipe, the pressure at the throat will be


less than that in the pipe, as prescribed by Bernoulli?s


equation, and consequently, the liquid in the throat


manometer elevations, together with a knowledge of the


cross-sections of pipe and throat, permit the liquid flow to


be measured. This device is known as a Venturi meter.


Bernoulli?s theorem is not only applicable for liquids,


but also for gasses. In this case, the mathematical


treatment is complicated by the fact that gases are highly


compressible, but the general effect is the same as


previously described; namely, that when a flowing stream of


gas speeds up, its pressure decreases, and vice versa.


The lift on an aircraft wing can be explained by this


effect. Airplane wings are designed so that the air speed


above the wing is greater than that below the wing. As a


result, the air pressure above the wing is less than the


pressure below, and there is a net upward force on the wing


called the ?lift?.


In conclusion, Bernoulli contributed much to the world


and to the realm of physics. Daniel Bernoulli derived a


fundamental expression that relates pressure to fluid speed


and elevation. Bernoulli?s equation is not a freestanding


law of physics, but instead a consequence of energy


conservation as applied to the ideal fluid.


References


Adiar, Robert. The Great Design: Particles, Fields and


Creation. New York: Oxford University Press, 1987.


Benton, William. ?Bernoulli, Daniel?. Encyclopedia


Britannic. 1969.


Duncan and Starling. A Textbook of Physics. London:


Macmillan and Co. 1948.


Furry, Purcell and Street. Physics. New York: Blankston


Co. 1952.

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