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Bernoulli equation and its physical applications (Topic)

The Bernoulli equation has the form

dy-
dx + f(x)y = g(x)yk (1)

where f and g are continuous real functions and k is a constant (0, 1). Such an equation is got e.g. in examining the motion of a body when the resistance of medium depends on the velocity v as

              k
F = λ1v +  λ2v .

The real function y can be solved from (1) explicitly. To do this, divide first both sides by yk. It yields

ykdy
---
dx + f(x)yk+1 = g(x). (2)

The substitution

z := yk+1 (3)

transforms (2) into

dz
---+ (− k + 1)f(x )z =  (− k + 1)g(x )
dx

which is a linear differential equation of first order. When one has obtained its general solution and made in this the substitution (3), then one has solved the Bernoulli equation (1).

References

[1]   N. Piskunov: Diferentsiaal- ja integraalarvutus kõrgematele tehnilistele õppeasutustele. – Kirjastus Valgus, Tallinn (1966).


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Cross-references: differential equation, motion, functions

This is version 1 of Bernoulli equation and its physical applications, born on 2009-04-18.
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Classification:
Physics Classification02.30.Hq (Ordinary differential equations)
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