Exact Equations

As remarked, there are no general methods to find a solution of (7.1.2). The EXACT EQUATIONS is yet another class of equations that can be easily solved. In this section, we introduce this concept.

Let $ D$ be a region in $ xy$ -plane and let $ M$ and $ N$ be real valued functions defined on $ D.$ Consider an equation

$\displaystyle M(x, y) + N(x, y) \frac{dy}{dx} = 0, \; (x, y) \in D.$ (7.3.1)

In most of the books on Differential Equations, this equation is also written as

$\displaystyle M(x, y) dx + N(x, y) dy = 0, \; (x, y) \in D.$ (7.3.2)

DEFINITION 7.3.1 (Exact Equation)   The Equation (7.3.1) is called Exact if there exists a real valued twice continuously differentiable function $ f: {\mathbb{R}}^2 {\longrightarrow}{\mathbb{R}}$ (or the domain is an open subset of $ {\mathbb{R}}^2$ ) such that

$\displaystyle \frac{\partial f}{\partial x} = M \; {\mbox{ and }} \; \frac{\partial f}{\partial y} = N.$ (7.3.3)

Remark 7.3.2   If (7.3.1) is exact, then

$\displaystyle \frac{\partial f}{\partial x} + \frac{\partial f}{\partial y} \cdot \frac{dy}{dx}
= \frac{df(x, y)}{dx} = 0.$

This implies that $ f(x,y) = c$ (where $ c$ is a constant) is an implicit solution of (7.3.1). In other words, the left side of (7.3.1) is an exact differential.

EXAMPLE 7.3.3   The equation $ y + x \frac{dy}{dx} = 0$ is an exact equation. Observe that in this example, $ f(x,y) = x y.$

The proof of the next theorem is given in Appendix 14.6.2.

THEOREM 7.3.4   Let $ M$ and $ N$ be twice continuously differentiable function in a region $ D.$ The Equation (7.3.1) is exact if and only if

$\displaystyle \frac{\partial M}{\partial y}= \frac{\partial N}{\partial x}.$ (7.3.4)

Note: If (7.3.1) or (7.3.2) is exact, then there is a function $ f(x,y)$ satisfying $ f(x,y) = c$ for some constant $ c,$ such that

$\displaystyle d( f(x, y) ) = M(x, y) dx + N(x,y) dy = 0.$

Let us consider some examples, where Theorem 7.3.4 can be used to easily find the general solution.

EXAMPLE 7.3.5  
  1. Solve

    $\displaystyle 2 x e^{y} + (x^2 e^{y} + \cos y \; )
\frac{dy}{dx} = 0.\;\;$


    Solution: With the above notations, we have

    $\displaystyle M = 2 x e^{y}, \; N = x^2 e^{y} + \cos y, \; \frac{\partial
M}{\...
...y} = 2 x e^{y} \; {\mbox{ and }} \; \frac{\partial
N}{\partial x} = 2 x e^{y}.$

    Therefore, the given equation is exact. Hence, there exists a function $ G(x,y)$ such that

    $\displaystyle \frac{\partial G}{\partial x} = 2 x e^{y} \;\;{\mbox{ and }}\;\;
\frac{\partial G}{\partial y} = x^2 e^{y} + \cos y.$

    The first partial differentiation when integrated with respect to $ x$ (assuming $ y$ to be a constant) gives,

    $\displaystyle G(x,y) = x^2 e^{y} +
h(y).$

    But then

    $\displaystyle \frac{\partial G}{\partial y} =
\frac{\partial (x^2 e^{y} + h(y))}{\partial y}
= N$

    implies $ \frac{dh}{dy} = \cos y$ or $ h(y) = \sin y + c$ where $ c$ is an arbitrary constant. Thus, the general solution of the given equation is

    $\displaystyle x^2 e^{y} + \sin y = c.$

    The solution in this case is in implicit form.
  2. Find values of $ \ell$ and $ m$ such that the equation

    $\displaystyle \ell y^2 + m x y \frac{dy}{dx} = 0$

    is exact. Also, find its general solution.
    Solution: In this example, we have

    $\displaystyle M = \ell y^2, \;
N = m x y, \; \; \frac{\partial M}{\partial y} = 2 \ell y\; {\mbox{ and }}
\; \frac{\partial N}{\partial x} = m y.$

    Hence for the given equation to be exact, $ m = 2 \ell.$ With this condition on $ \ell$ and $ m,$ the equation reduces to

    $\displaystyle \ell y^2 + 2 \ell x y \frac{dy}{dx} = 0.$

    This equation is not meaningful if $ \ell = 0.$ Thus, the above equation reduces to

    $\displaystyle \frac{d}{dx}(x y^2) = 0$

    whose solution is

    $\displaystyle x y^2 = c$

    for some arbitrary constant $ c.$
  3. Solve the equation

    $\displaystyle (3 x^2 e^{y} - x^2 ) dx + (x^3 e^{y} + y^2)
dy = 0.$


    Solution: Here

    $\displaystyle M = 3 x^2 e^{y} - x^2 \; {\mbox{ and }}\;
N = x^3 e^{y} + y^2.$

    Hence, $ \frac{\partial M}{\partial y} =
\frac{\partial N}{\partial x} = 3 x^2 e^{y}.$ Thus the given equation is exact. Therefore,

    $\displaystyle G(x, y) = \int (3 x^2 e^{y} - x^2) d x = x^3 e^{y} -
\frac{x^3}{3} + h(y)$

    (keeping $ y$ as constant). To determine $ h(y),$ we partially differentiate $ G(x,y)$ with respect to $ y$ and compare with $ N$ to get $ h(y) = \frac{y^3}{3}.$ Hence

    $\displaystyle G(x,y) = x^3 e^{y} - \frac{x^3}{3} + \frac{y^3}{3} = c$

    is the required implicit solution.



Subsections
A K Lal 2007-09-12