Miscellaneous Remarks

In Section 7.4, we have learned to solve the linear equations. There are many other equations, though not linear, which are also amicable for solving. Below, we consider a few classes of equations which can be solved. In this section or in the sequel, $ p$ denotes $ \displaystyle\frac{dy}{dx}$ or $ y^\prime.$ A word of caution is needed here. The method described below are more or less ad hoc methods.

  1. EQUATIONS SOLVABLE FOR Y:
    Consider an equation of the form

    $\displaystyle y = f(x,p).$ (7.5.1)

    Differentiating with respect to $ x,$ we get

    $\displaystyle \frac{dy}{dx} = p = \frac{\partial f(x,p)}{\partial x} + \frac{\...
...dot \frac{dp}{dx} \; {\mbox{ of equivalently }} \;\;p = g(x,p, \frac{dp}{dx}).$ (7.5.2)

    The Equation (7.5.2) can be viewed as a differential equation in $ p$ and $ x.$ We now assume that (7.5.2) can be solved for $ p$ and its solution is

    $\displaystyle h(x, p, c) = 0.$ (7.5.3)

    If we are able to eliminate $ p$ between (7.5.1) and (7.5.3), then we have an implicit solution of the (7.5.1).

    Solve $ y = 2 p x - x p^2.$
    Solution: Differentiating with respect to $ x$ and replacing $ \displaystyle\frac{dy}{dx}$ by $ p,$ we get

    $\displaystyle p = 2p - p^2
+ 2x \frac{dp}{dx} - 2x p \frac{dp}{dx} \;\; {\mbox{ or }} \;\;
(p + 2 x \frac{dp}{dx}) (1-p) = 0.$

    So, either

    $\displaystyle p + 2 x \frac{dp}{dx} = 0 \;\; {\mbox{ or }} \;\; p = 1.$

    That is, either $ p^2 x = c$ or $ p=1.$ Eliminating $ p$ from the given equation leads to an explicit solution

    $\displaystyle y = 2 x \sqrt{\frac{c}{x}} - c \; {\mbox{ or }} \;\;
y = x.$

    The first solution is a one-parameter family of solutions, giving us a general solution. The latter one is a solution but not a general solution since it is not a one parameter family of solutions.

  2. EQUATIONS IN WHICH THE INDEPENDENT VARIABLE MATHEND000# IS MISSING:
    These are equations of the type $ f(y, p) = 0.$ If possible we solve for $ y$ and we proceed. Sometimes introducing an arbitrary parameter helps. We illustrate it below.

    Solve $ y^2 + p^2 = a^2$ where $ a$ is a constant.
    Solution: We equivalently rewrite the given equation, by (arbitrarily) introducing a new parameter $ t$ by

    $\displaystyle y = a \sin t, \;\; p = a
\cos t$

    from which it follows

    $\displaystyle \frac{dy}{dt} = a \cos t; \;\; p
= \frac{dy}{dx}= \frac{dy}{dt}\biggl/\frac{dx}{dt}\biggr.$

    and so

    $\displaystyle \frac{dx}{dt} = \frac{1}{p} \frac{dy}{dt} = 1\;\; {\mbox{ or }} \;\;
x = t + c.$

    Therefore, a general solution is

    $\displaystyle y = a \sin (t+c).$

  3. EQUATIONS IN WHICH MATHEND000# (DEPENDENT VARIABLE OR THE UNKNOWN) IS MISSING:
    We illustrate this case by an example.

    Find the general solution of $ x = p^3 - p - 1.$
    Solution: Recall that $ p
= \frac{dy}{dx}.$ Now, from the given equation, we have

    $\displaystyle \frac{dy}{dp}= \frac{dy}{dx}\cdot\frac{dx}{dp}=
p (3p^2 - 1).$

    Therefore,

    $\displaystyle y = \frac{3}{4} p^4 - \frac{1}{2} p^2 + c$

    (regarding $ p$ as a parameter). The desired solution in this case is in the parametric form, given by

    $\displaystyle x = t^3 - t - 1 \;\; {\mbox{ and }} y
= \frac{3}{4} t^4 - \frac{1}{2} t^2 + c$

    where $ c$ is an arbitrary constant.

    Remark 7.5.1   The readers are again informed that the methods discussed in $ 1), 2), 3)$ are more or less ad hoc methods. It may not work in all cases.

EXERCISE 7.5.2  
  1. Find the general solution of $ y = (1 + p ) x + p^2.$
    Hint: Differentiate with respect to $ x$ to get $ \displaystyle\frac{dx}{dp} = - (x + 2 p)$ ( a linear equation in $ x$ ). Express the solution in the parametric form

    $\displaystyle y(p) = (1 + p) x + p^2, \;\;
x(p) = 2(1-p) + c e^{-p}.$

  2. Solve the following differential equations:
    1. $ 8 y = x^2 + p^2.$
    2. $ y + x p = x^4 p^2.$
    3. $ y^2 \log y - p^2 = 2 x y p.$
    4. $ 2 y + p^2 + 2 p = 2 x (p+1).$
    5. $ 2 y = 2 x^2 + 4 p x + p^2.$

A K Lal 2007-09-12