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Bernoulli’s Equation is considered one the most difficult concept.
9 Questions around this concept.
Let $y=y(x)$ be the solution of the differential equation $\frac{d y}{d x}=\frac{(\tan x)+y}{\sin x(\sec x-\sin x \tan x)}, x \in\left(0, \frac{\pi}{2}\right)$ satisfying the condition $y\left(\frac{\pi}{4}\right)=2$. Then, $y\left(\frac{\pi}{3}\right)$ is
The temperature $\mathrm{T}(\mathrm{t})$ of a body at time $\mathrm{t}=0$ is $160^{\circ} \mathrm{F}$ and it decreases continuously as per the differential equation $\frac{\mathrm{dT}}{\mathrm{dt}}=-\mathrm{K}(\mathrm{T}-80)$, where $\mathrm{K}$ is a positive constant. If $\mathrm{T}(15)=120^{\circ} \mathrm{F}$, then $\mathrm{T}(45)$ is equal to
When DE is not in the linear form, it can sometimes be converted into a linear form with the help of proper substitution.
An equation of the form
$
\frac{\mathrm{dy}}{\mathrm{dx}}+\mathrm{P}(\mathrm{x}) \cdot \mathrm{y}=\mathrm{Q}(\mathrm{x}) \cdot \mathrm{y}^{\mathrm{n}}
$
Where $\mathrm{P}(\mathrm{x})$ and $\mathrm{Q}(\mathrm{x})$ are a function of x only, is known as Bernoulli's equation.
(If we put $\mathrm{n}=0$, then the equation is in linear form.)
To reduce Eq (i) into linear form, divide both sides by $\mathrm{y}^{\mathrm{n}}$,
$
\begin{gathered}
\frac{1}{y^n} \cdot \frac{d y}{d x}+\frac{P(x)}{y^{n-1}}=Q(x) \\
\text { or } \quad y^{-n} \cdot \frac{d y}{d x}+y^{1-n} \cdot P(x)=Q(x)
\end{gathered}
$
Putting $y^{1-n}=t$, converts this equation into a linear equation in $t$, which can then be solved
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