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Class 02

Example ii:
We are given:

\[ \frac{dy}{dx} = e^x \left( A\sin 2x + B\cos 2x \right) + e^x \left[ A\cos 2x \cdot 2 + B(-\sin 2x) \cdot 2 \right] \]

This simplifies to:

\[ \frac{dy}{dx} = y + e^x \left( 2A\cos 2x - 2B\sin 2x \right) \tag{1} \]

Now, differentiating again with respect to \(x\):

\[ \frac{d^2y}{dx^2} = y' + e^x \left[ 2(-2A\sin 2x) - 2(2B\cos 2x) \right] \]
\[ \quad\quad\quad\; + e^x \left( 2A\cos 2x - 2B\sin 2x \right) + \frac{dy}{dx} \]

From equation (1), substituting \(e^x(2A\cos 2x - 2B\sin 2x) = \frac{dy}{dx} - y\), we get:

\[ \frac{d^2y}{dx^2} = -4y + \left( \frac{dy}{dx} - y \right) + \frac{dy}{dx} \]

Simplifying:

\[ \frac{d^2y}{dx^2} = -4y + 2\frac{dy}{dx} - y \]
\[ \frac{d^2y}{dx^2} + 5y - 2\frac{dy}{dx} = 0 \]

Hence,

\[ \boxed{\frac{d^2y}{dx^2} - 2\frac{dy}{dx} + 5y = 0} \]

is the required differential equation.


Example:
Show that \(Ax^2 + By^2 = 1\) is the solution of

\[ x \left\{ y \frac{d^2 y}{dx^2} + \left( \frac{dy}{dx} \right)^2 \right\} = y \frac{dy}{dx} \]

Solution:
Given:

\[ Ax^2 + By^2 = 1 \]

Differentiating with respect to \(x\):

\[ A \cdot 2x + B \cdot 2y \frac{dy}{dx} = 0 \]
\[ 2Ax + 2By \frac{dy}{dx} = 0 \]
\[ Ax + By \frac{dy}{dx} = 0 \]
\[ Ax = -B y \frac{dy}{dx} \]
\[ -\frac{A}{B} = \frac{y}{x} \cdot \frac{dy}{dx} \]

Differentiating again:

\[ 0 = \frac{y}{x} \cdot \frac{d^2y}{dx^2} + \frac{dy}{dx} \cdot \frac{x \frac{dy}{dx} - y}{x^2} \]

Multiplying through by \(x^2\):

\[ y \cdot x \frac{d^2y}{dx^2} + x \left( \frac{dy}{dx} \right)^2 - y \frac{dy}{dx} = 0 \]
\[ xy \frac{d^2y}{dx^2} + x \left( \frac{dy}{dx} \right)^2 - y \frac{dy}{dx} = 0 \]

Thus,

\[ x \left\{ y \frac{d^2 y}{dx^2} + \left( \frac{dy}{dx} \right)^2 \right\} = y \frac{dy}{dx} \]

Hence proved. \(\quad \text{(Shown)}\) ✅


Short Question: Concentric Circle Whose Centre is the OriginÂļ

226x202
1.
A concentric circle with its centre at the origin has the general equation:

\[ x^2 + y^2 = a^2 \]

Differentiating with respect to \(x\), we get:

\[ x + y \frac{dy}{dx} = 0 \]

which is the required differential equation.


2. For a general circle (not necessarily concentric), the equation is:

\[ x^2 + y^2 + 2gx + 2fy + c = 0 \]

Here, the Centre is \((-g, -f)\).


āφāĻŽāϰāĻž āφāϗ⧇ concept clear āĻ•āϰāĻŦ, āϤāĻžāϰāĻĒāϰ equation derive āĻ•āϰāĻŦāĨ¤

1ī¸âƒŖ Problem-āϟāĻž āφāϏāϞ⧇ āϕ⧀ āĻŦāϞāϛ⧇?Âļ

āφāĻŽāϰāĻž āĻāĻ•āϟāĻž family of circles āύāĻŋā§Ÿā§‡ āĻ•āĻĨāĻž āĻŦāϞāĻ›āĻŋāĨ¤
āĻāχ circles āϗ⧁āϞ⧋ special —

  • āĻāϗ⧁āϞ⧋ x-axis-āϕ⧇ (horizontal axis) origin (0,0)-āĻ touch āĻ•āϰāϛ⧇āĨ¤
  • Circle-āĻāϰ center āϏāĻŦāϏāĻŽā§Ÿ y-axis-āĻāϰ āωāĻĒāϰ⧇ āĻĨāĻžāĻ•āĻŦ⧇āĨ¤

📌 āĻŽāĻžāύ⧇, āĻāϗ⧁āϞ⧋ āĻāĻŽāύ āĻšāĻŦ⧇ ↓
(āĻāĻ•āϟāĻž circle āωāĻĒāϰ⧇, āϝ⧇āϟāĻž x-axis-āĻāϰ āωāĻĒāϰ āĻļ⧁āϧ⧁ āĻāĻ• āĻĒā§Ÿā§‡āĻ¨ā§āĻŸā§‡ āĻ¸ā§āĻĒāĻ°ā§āĻļ āĻ•āϰāϛ⧇, āύāĻŋāĻšā§‡ āϝ⧇āϤ⧇ āĻĒāĻžāϰāϛ⧇ āύāĻž)


2ī¸âƒŖ āϕ⧇āύ center y-axis-āĻ?Âļ

āĻ•āĻžāϰāĻŖ:
āϝāĻĻāĻŋ circle origin-āĻ x-axis-āϕ⧇ āĻ¸ā§āĻĒāĻ°ā§āĻļ āĻ•āϰ⧇, symmetry-āĻāϰ āĻ•āĻžāϰāϪ⧇ center āĻ…āĻŦāĻļā§āϝāχ x=0 āϞāĻžāχāύ (y-axis)-āĻ āĻšāĻŦ⧇āĨ¤
āϧāϰāĻŋ center = \((0,a)\), radius = \(a\) (āĻ•āĻžāϰāĻŖ center āĻĨ⧇āϕ⧇ x-axis āĻĒāĻ°ā§āϝāĻ¨ā§āϤ vertical distance = a, āϝāĻž radius)āĨ¤


3ī¸âƒŖ Circle-āĻāϰ Equation āϞāĻŋāĻ–āĻŋÂļ

Center (0,a), radius a ⇒ equation āĻšāĻŦ⧇:

\[ (x-0)^2 + (y-a)^2 = a^2 \]

āϏ⧇āϟāĻž expand āĻ•āϰāϞ⧇:

\[ x^2 + y^2 - 2ay = 0 \]

āĻāĻ–āĻžāύ⧇ a āĻšāϞ⧋ āφāĻŽāĻžāĻĻ⧇āϰ parameter (āĻĒā§āϰāϤāĻŋāϟāĻž circle-āĻāϰ āϜāĻ¨ā§āϝ āφāϞāĻžāĻĻāĻž)āĨ¤


4ī¸âƒŖ āĻāĻ–āύ Derivative āύ⧇āχÂļ

āφāĻŽāϰāĻž āϚāĻžāχ differential equation, āĻŽāĻžāύ⧇ parameter a āϕ⧇ āĻŦāĻžāĻĻ āĻĻāĻŋā§Ÿā§‡ x, y, dy/dx-āĻāϰ relationāĨ¤

Equation:

\[ x^2 + y^2 - 2ay = 0 \]

Differentiating wrt x:

\[ 2x + 2y \frac{dy}{dx} - 2a \frac{dy}{dx} = 0 \]

2 āĻĻāĻŋā§Ÿā§‡ āĻ­āĻžāĻ— āĻ•āϰāϞ⧇:

\[ x + (y-a) y' = 0 \]

āĻāĻ–āĻžāύ⧇ \(y' = \frac{dy}{dx}\)āĨ¤

5ī¸âƒŖ a āϕ⧇ eliminate āĻ•āϰāĻŋÂļ

Original equation āĻĨ⧇āϕ⧇:

\[ 2ay = x^2 + y^2 \quad\Rightarrow\quad a = \frac{x^2 + y^2}{2y} \]

āĻāĻ–āύ \(y-a\) āĻŦ⧇āϰ āĻ•āϰāĻŋ:

\[ y-a = y - \frac{x^2 + y^2}{2y} = \frac{2y^2 - (x^2 + y^2)}{2y} = \frac{y^2 - x^2}{2y} = -\frac{x^2 - y^2}{2y} \]

6ī¸âƒŖ Back to derivative equationÂļ

\(y-a = -\frac{x^2 - y^2}{2y}\) āĻāϟāĻž \(x + (y-a)y' = 0\)-āĻ āĻŦāϏāĻžāχ:

\[ x - \frac{x^2 - y^2}{2y} y' = 0 \]

Multiply by \(2y\):

\[ 2xy - (x^2 - y^2) y' = 0 \]

Rearrange:

\[ (x^2 - y^2) y' - 2xy = 0 \]

y' āĻāϰ āϜāĻžā§ŸāĻ—āĻžā§Ÿ \(\frac{dy}{dx}\) āϞāĻŋāĻ–āϞ⧇:

\[ (x^2 - y^2) \frac{dy}{dx} - 2xy = 0 \]

Cross-multiply āĻ•āϰāϞ⧇:

\[ \boxed{(x^2 - y^2) dy - 2xy dx = 0} \]

Family of Circles Touching the x‑Axis at the Origin — Differential Equation

✅ āĻāϟāĻžāχ āĻšā§‡ā§Ÿā§‡āĻ›āĻŋāϞāĨ¤
āĻŦā§‹āĻāĻžāϰ āϞāϜāĻŋāĻ•:

  • Geometry āĻĨ⧇āϕ⧇ center āύāĻŋāĻ°ā§āϧāĻžāϰāĻŖ āĻ•āϰ⧋
  • Equation āϞ⧇āĻ–ā§‹
  • Differentiate āĻ•āϰ⧇ parameter āĻŦāĻžāĻĻ āĻĻāĻžāĻ“
  • Final differential equation āĻĒā§‡ā§Ÿā§‡ āϝāĻžāĻ“

Example:Âļ

Show that the differential equation of a family of circles touching the \(x\)-axis at the origin is

\[ (x^2 - y^2) \, dy - 2xy \, dx = 0 \]

Solution:

The equation of a family of circles touching the \(x\)-axis at the origin is:

\[ x^2 + y^2 + 2fy + c = 0 \]

Since the circle passes through \((0,0)\),

\[ c = 0 \]

Thus,

\[ x^2 + y^2 + 2fy = 0 \quad \cdots (1) \]

Step 1: Differentiate w.r.to \(x\)Âļ

Differentiating (1):

\[ 2x + 2y \frac{dy}{dx} + 2f \frac{dy}{dx} = 0 \]

Divide by 2:

\[ x + y \frac{dy}{dx} + f \frac{dy}{dx} = 0 \quad \cdots (2) \]

Step 2: Eliminate \(f\)Âļ

From (1):

\[ f = -\frac{x^2 + y^2}{2y} \]

Substitute in (2):

\[ x + y \frac{dy}{dx} - \frac{x^2 + y^2}{2y} \cdot \frac{dy}{dx} = 0 \]

Step 3: SimplifyÂļ

Multiply through by \(2y\):

\[ 2xy + 2y^2 \frac{dy}{dx} - (x^2 + y^2) \frac{dy}{dx} = 0 \]
\[ 2xy + 2y^2 \frac{dy}{dx} - x^2 \frac{dy}{dx} - y^2 \frac{dy}{dx} = 0 \]
\[ 2xy + y^2 \frac{dy}{dx} - x^2 \frac{dy}{dx} = 0 \]

Step 4: RearrangeÂļ

\[ 2xy \, dx + (y^2 - x^2) dy = 0 \]

Multiply by \(-1\):

\[ (x^2 - y^2) dy - 2xy \, dx = 0 \]

✅ Hence proved:

\[ \boxed{(x^2 - y^2) \, dy - 2xy \, dx = 0} \]

H.W.: Find the differential equation of a family of circles touching the \(y\)-axis.


H.W.–2:
Show that the differential equation of a family of circles

\[ x^2 + y^2 + 2gx + 2fy + c = 0 \]

is

\[ (1 + y'^2) y_3 - 3y' y''^2 = 0 \]

Practice Problem — Find Order & Degree

Given equation:

\[ \sqrt[3]{\left(\frac{d^3y}{dx^3}\right)^4 - 5x\frac{d^2y}{dx^2} + y} = \sqrt[5]{\left(\frac{dy}{dx}\right)^2 + y^2 - x} \]

Step 1: OrderÂļ

  • The highest order derivative present is \(\frac{d^3y}{dx^3}\).
  • Therefore, Order = 3.

Step 2: DegreeÂļ

  • The cube root applies to the entire left-hand side expression, and the fifth root applies to the entire right-hand side.
  • Remove both roots by raising both sides to the 15th power (LCM of 3 and 5):
\[ \left[\left(\frac{d^3y}{dx^3}\right)^4 - 5x\frac{d^2y}{dx^2} + y\right]^5 = \left[\left(\frac{dy}{dx}\right)^2 + y^2 - x\right]^3 \]
  • Now, the highest derivative term becomes:
\[ \left(\frac{d^3y}{dx^3}\right)^{4 \times 5} = \left(\frac{d^3y}{dx^3}\right)^{20} \]
  • Hence, Degree = 20.

Final Answer:

\[ \boxed{\text{Order} = 3, \quad \text{Degree} = 20} \]

Differential Equation of First Order and First Degree

The most general form of an ordinary differential equation of the 1st order and 1st degree is:

\[ M\,dx + N\,dy = 0 \]

or equivalently,

\[ N \frac{dy}{dx} + M = 0 \]

where both \(M\) and \(N\) are functions of \(x\) and \(y\), or constants, and do not involve any derivatives.


Solution Methods:

  1. Separation of Variables – Variables are separated so that all \(x\) terms are on one side and all \(y\) terms on the other.
  2. Homogeneous Equation – Equation in which \(M\) and \(N\) are homogeneous functions of the same degree.
  3. Equation Reducible to Homogeneous Form – Transformed into homogeneous type by substitution.
  4. Exact Equation – Condition: \(\frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}\).
  5. Linear Equation – Follows the form \(\frac{dy}{dx} + P(x)y = Q(x)\).
  6. Equation Reducible to Linear Form – Can be rearranged into the linear equation format.

Example 1 — Separation of Variables

Solve:

\[ x^2 (y - 1)\, dx + y^2 (x - 1)\, dy = 0 \]

Solution:
Given:

\[ x^2 (y - 1)\, dx + y^2 (x - 1)\, dy = 0 \]

Divide through by \((x - 1)(y - 1)\):

\[ \frac{x^2}{x - 1}\, dx + \frac{y^2}{y - 1}\, dy = 0 \]

Rewrite:

\[ \left(x + 1 + \frac{1}{x - 1}\right) dx + \left(y + 1 + \frac{1}{y - 1}\right) dy = 0 \]

Integrate both sides:

\[ \int x\, dx + \int 1\, dx + \int \frac{1}{x - 1} dx + \int y\, dy + \int 1\, dy + \int \frac{1}{y - 1} dy = C \]
\[ \frac{x^2}{2} + x + \log|x - 1| + \frac{y^2}{2} + y + \log|y - 1| = C \]

Multiply by 2 (or combine constants):

\[ x^2 + y^2 + 2x + 2y + \log(x - 1) + \log(y - 1) = C \]

where \(C\) is an arbitrary constant.


Example — 2
Solve:

\[ \frac{dy}{dx} = e^{x+y} + x^2 e^{-y} \]

Solution:

\[ \frac{dy}{dx} = e^x \cdot e^y + x^2 \cdot e^{-y} \]

Actually, write directly:

\[ e^y \frac{dy}{dx} = e^x + x^2 \]

Now integrate both sides with respect to \(x\):

\[ \int e^y \, dy = \int e^x \, dx + \int x^2 \, dx \]
\[ e^y = e^x + \frac{x^3}{3} + C \]

HW-02

❓H.W.–2:
Show that the differential equation of a family of circles

\[ x^2 + y^2 + 2gx + 2fy + c = 0 \]

(āĻāϟāĻž āĻšāϞ general equation of a circle, āϝ⧇āĻ–āĻžāύ⧇ g, f, c constant — different circles āĻāϰ āϜāĻ¨ā§āϝ g, f, c āĻāϰ āĻŽāĻžāύ āφāϞāĻžāĻĻāĻž āĻšāϤ⧇ āĻĒāĻžāϰ⧇)

is

\[ (1 + y_1^{\,2})\,y_3 - 3y_1\,y_2^{\,2} = 0, \]

(āφāĻŽāĻžāĻĻ⧇āϰ āϞāĻ•ā§āĻˇā§āϝ āĻāχ form-āϟāĻž āĻĒā§āϰāĻŽāĻžāĻŖ āĻ•āϰāĻž, āϝ⧇āĻ–āĻžāύ⧇ \(y_1, y_2, y_3\) āĻšāϞ⧋ āĻĒā§āϰāĻĨāĻŽ, āĻĻā§āĻŦāĻŋāĻ¤ā§€ā§Ÿ āĻ“ āϤ⧃āĻ¤ā§€ā§Ÿ derivative)

where \(y_1=\dfrac{dy}{dx},\; y_2=\dfrac{d^2y}{dx^2},\; y_3=\dfrac{d^3y}{dx^3}\).


Given family:

\[ x^2+y^2+2gx+2fy+c=0 \quad (g,f,c \text{ constants}) \]

1st derivative → \(x+yy_1+g+fy_1=0\) â€Ļ (A)
(āĻāĻ–āĻžāύ⧇ āĻĻ⧁āχ āĻĒāĻžāĻļ⧇ \(d/dx\) āĻ•āϰāϞāĻžāĻŽ; \(y^2\) āĻāϰ derivative = \(2y \cdot y_1\), āφāĻŦāĻžāϰ \(2fy\) āĻāϰ derivative = \(2f \cdot y_1\), āϤāĻžāϰāĻĒāϰ 2 āĻĻāĻŋā§Ÿā§‡ divide āĻ•āϰāĻžā§Ÿ āĻāχ āĻĢāĻ°ā§āĻŽ āĻĒ⧇āϞāĻžāĻŽ)

2nd derivative → \(1+y_1^2+yy_2+fy_2=0\)

(āφāĻŦāĻžāϰ derivative āĻ•āϰāϞāĻžāĻŽ; \(y y_1\) āĻāϰ derivative = \(y_1^2 + y y_2\))

\[ \Rightarrow\ (y+f)\,y_2=-(1+y_1^2) \quad\text{â€Ļ (B)} \]

(āĻāĻ–āĻžāύ⧇ \(y_2\) āĻāϰ term āϗ⧁āϞ⧋ āĻāĻ•āϏāĻžāĻĨ⧇ āĻ•āϰ⧇, \(y+f\) factor āĻšāĻŋāϏ⧇āĻŦ⧇ āĻŦ⧇āϰ āĻ•āϰ⧇ āύāĻŋāϞāĻžāĻŽ)

3rd derivative of (2nd) → \(3y_1y_2+(y+f)\,y_3=0\) â€Ļ (C)

(āĻāĻŦāĻžāϰ āĻĻā§āĻŦāĻŋāĻ¤ā§€ā§Ÿ derivative āϏāĻŽā§€āĻ•āϰāĻŖāϟāĻžāϰ derivative āĻ•āϰāϞāĻžāĻŽ; \(y_1^2\) āĻāϰ derivative = \(2y_1y_2\), āϏāĻžāĻĨ⧇ \((y+f) y_2\) āĻāϰ derivative āĻĻāĻŋāϞ⧇ \(y_1 y_2 + (y+f) y_3\) — āϏāĻŦ āĻŽāĻŋāϞ⧇ \(3y_1 y_2 + (y+f) y_3\))

(B) āĻĨ⧇āϕ⧇ \((y+f)=-(1+y_1^2)/y_2\) āĻŦāϏāĻŋā§Ÿā§‡ (C):
(āφāϗ⧇āϰ āϧāĻžāĻĒ⧇āϰ (B) āĻĨ⧇āϕ⧇ \(y+f\) āĻāϰ āĻŽāĻžāύ āύāĻŋāϞāĻžāĻŽ āĻāĻŦāĻ‚ (C)-āϤ⧇ āĻŦāϏāĻžāϞāĻžāĻŽ)

\[ 3y_1y_2-\frac{1+y_1^2}{y_2}\,y_3=0 \]

(āĻāĻ–āĻžāύ⧇ \(y+f\) āĻāϰ āϜāĻžā§ŸāĻ—āĻžā§Ÿ fraction āĻŦāϏ⧇āϛ⧇, āφāϰ minus sign āϕ⧇ adjust āĻ•āϰ⧇ āĻāχ āĻĢāĻ°ā§āĻŽ āĻāϏ⧇āϛ⧇)

\[ \boxed{(1+y_1^2)\,y_3-3y_1\,y_2^2=0} \]

(āĻļ⧇āώ⧇ rearrange āĻ•āϰ⧇ āĻ āĻŋāĻ• āφāĻŽāĻžāĻĻ⧇āϰ āĻĒā§āϰāĻŽāĻžāĻŖ āĻ•āϰāϤ⧇ āϚāĻžāĻ“ā§ŸāĻž final equation āĻĒ⧇āϞāĻžāĻŽ ✅)