Solve the differential equation
\frac {t}{y} \acute{y}+ln(ty)+1 = 0
Solve the differential equation
\frac {t}{y} \acute{y}+ln(ty)+1 = 0
We begin by observing that this equation is neither linear nor separable. Thus, writing the derivative in differential notation, we have
\frac {t}{y} \frac {dy}{dt}+ln(ty)+1 = 0
and then rearranging algebraically,
(ln(ty)+1)dt + \frac {t}{y} dy = 0 (2.5.10)
Letting M(t , y) = ln(ty)+1 and N(t , y) = t /y, we observe that
M_{y} =\frac {1}{ty} t=\frac {1}{y} and N_{t} =\frac {1}{y}
and therefore, M_{y} = N_{t} . Hence the differential equation is exact and we can assume that a function φ exists such that φ_{t} =M(t , y) and φ_{y} = N(t , y).
the latter equation is more elementary, we consider φ_{y} = t /y, and integrate both sides with respect to y. Doing so, we find that
φ(t , y) = t ln y +h(t) (2.5.11)
From (2.5.10), φ must also satisfy φ_{t} =ln(ty)+1, so we take the partial derivative of both sides of (2.5.11) with respect to t to find that
φ_{t} = ln y +h´(t ) = ln(ty)+1
From this and properties of the logarithm, we observe that
ln y +h´(t ) = ln t +ln y +1
and thus h´(t ) = ln t +1. It follows (integrating by parts and simplifying) that h(t ) = t ln t . Thus, we have demonstrated that the original equation is indeed exact by finding φ(t , y)=t ln y +t ln t =t ln(ty). From here, we now know that φ(t , y) = K, and so
t ln(ty) = K
Solving for y, we have that
y =\frac {1}{t} e^{K/t}