Chapter 9: Differential Equations
An equation involving derivatives (or differentials) of the dependent variable with respect to independent variable (or variables) is termed as a differential equation.
Order and Degree of a Differential Equation
- Order: The order of a differential equation is the order of the highest order derivative occurring in the differential equation.
- Degree: The degree of a differential equation is the highest power (positive integral index) of the highest order derivative occurring in it, after it has been expressed as a polynomial of derivatives.
Solutions of Differential Equations
A function which satisfies the given differential equation is called its solution.
- General Solution: The solution which contains arbitrary constants is called the general solution (primitive) of the differential equation.
- Particular Solution: The solution obtained from the general solution by giving particular values to the arbitrary constants is called a particular solution of the differential equation.
Methods of finding the solution of First Order First Degree Differential Equations:
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Differential Equations with Variables Separable: If the equation $\frac{dy}{dx} = f(x, y)$ can be written in the form $g(y)dy = h(x)dx$, integrating both sides gives the solution: $\int g(y)dy = \int h(x)dx + C$.
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Homogeneous Differential Equations: An equation $\frac{dy}{dx} = F(x, y)$ is said to be homogeneous if $F(x, y)$ is a homogeneous function of degree zero. To solve it, we make the substitution $y = vx$. Then $\frac{dy}{dx} = v + x\frac{dv}{dx}$ and the equation gets reduced to the separable form.
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Linear Differential Equations: Equations of the form $\frac{dy}{dx} + Py = Q$, where $P$ and $Q$ are functions of $x$ or constants. Integrating Factor (I.F.) = $e^{\int P dx}$. The solution is given by: $y \times \text{I.F.} = \int (Q \times \text{I.F.}) dx + C$.
Competency-Based Questions
1. [CBSE 2021] Find the specific solution of the differential equation $\cos(x) \frac{dy}{dx} + y \sin x = 1$, given that $y = 1$ when $x = 0$.
Solution:
$\cos x \frac{dy}{dx} + y \sin x = 1$
Divide by $\cos x$:
$\frac{dy}{dx} + y \tan x = \sec x$.
This is a linear differential equation of the form $\frac{dy}{dx} + Py = Q$.
Here, $P = \tan x$, $Q = \sec x$.
Integrating Factor (I.F.) $= e^{\int P dx} = e^{\int \tan x dx} = e^{\log|\sec x|} = \sec x$.
The general solution is:
$y \times \text{I.F.} = \int (Q \cdot \text{I.F.}) dx + C$
$y \sec x = \int (\sec x \cdot \sec x) dx + C$
$y \sec x = \int \sec^2 x dx + C$
$y \sec x = \tan x + C$.
Now, to find the specific solution, use the initial conditions: $y = 1$ when $x = 0$.
$(1) \sec(0) = \tan(0) + C$
$1 \times 1 = 0 + C \implies C = 1$.
Therefore, the specific solution is $y \sec x = \tan x + 1$ or $y = \sin x + \cos x$.
2. [Sample Paper 2022] Solve the differential equation $\frac{dy}{dx} = e^{x+y}$.
Solution:
$\frac{dy}{dx} = e^{x+y} = e^x \cdot e^y$
This is a separable variables equation.
$\frac{dy}{e^y} = e^x dx$
$e^{-y} dy = e^x dx$
Integrating both sides:
$\int e^{-y} dy = \int e^x dx$
$-e^{-y} = e^x + C_1$
$e^x + e^{-y} = -C_1$
Let $C = -C_1$, an arbitrary constant.
$e^x + e^{-y} = C$ is the general solution.
3. [CBSE 2019] Show that the differential equation $(x - y) \frac{dy}{dx} = x + 2y$ is homogeneous and solve it.
Solution:
$\frac{dy}{dx} = \frac{x + 2y}{x - y} = F(x, y)$
Let $x \to \lambda x$, $y \to \lambda y$: $F(\lambda x, \lambda y) = \frac{\lambda x + 2\lambda y}{\lambda x - \lambda y} = \frac{\lambda(x + 2y)}{\lambda(x - y)} = \lambda^0 F(x, y)$.
So, it is a homogeneous differential equation.
To solve, put $y = vx$. Then $\frac{dy}{dx} = v + x \frac{dv}{dx}$.
Substituting into the equation:
$v + x \frac{dv}{dx} = \frac{x + 2vx}{x - vx} = \frac{x(1 + 2v)}{x(1 - v)} = \frac{1 + 2v}{1 - v}$
$x \frac{dv}{dx} = \frac{1 + 2v}{1 - v} - v = \frac{1 + 2v - v(1 - v)}{1 - v} = \frac{1 + 2v - v + v^2}{1 - v}$
$x \frac{dv}{dx} = \frac{v^2 + v + 1}{1 - v}$
Separating variables:
$\frac{1 - v}{v^2 + v + 1} dv = \frac{dx}{x}$
Multiply by 2 for the numerator to become the derivative of denominator:
$\frac{2 - 2v}{v^2 + v + 1} dv = \frac{2}{x} dx$
$\frac{3 - (2v + 1)}{v^2 + v + 1} dv = \frac{2}{x} dx$
$\int \frac{3}{v^2 + v + 1} dv - \int \frac{2v + 1}{v^2 + v + 1} dv = \int \frac{2}{x} dx$
$\int \frac{3}{(v + 1/2)^2 + (\sqrt{3}/2)^2} dv - \log|v^2 + v + 1| = 2 \log|x| + C$
$3 \cdot \frac{1}{\sqrt{3}/2} \tan^{-1}\left(\frac{v + 1/2}{\sqrt{3}/2}\right) = \log|v^2 + v + 1| + \log x^2 + C$
$2\sqrt{3} \tan^{-1}\left(\frac{2v + 1}{\sqrt{3}}\right) = \log|x^2(v^2 + v + 1)| + C$
Substitute $v = y/x$:
$2\sqrt{3} \tan^{-1}\left(\frac{2y/x + 1}{\sqrt{3}}\right) = \log|x^2(y^2/x^2 + y/x + 1)| + C$
$2\sqrt{3} \tan^{-1}\left(\frac{2y + x}{\sqrt{3}x}\right) = \log|y^2 + xy + x^2| + C$.