The Bernoulli equation has the form
+ 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
The real function y can be solved from (1) explicitly. To do this, divide first both sides by yk. It
yields
y−k + f(x)y−k+1 = g(x). | | (2) |
The substitution
transforms (2) into
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).