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Ordinary Differential Equations and Exact Equations

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This document covers various topics in ordinary differential equations, focusing on first-order equations. It includes sections on linear and Bernoulli's differential equations, exact and reducible to exact equations, orthogonal trajectories, and applications in electrical circuits. The material provides detailed explanations of solution methods for different equation types, including linear, Bernoulli, and Clairaut's equations. It also discusses non-linear differential equations and presents numerous solved problems illustrating the application of these methods. Additionally, the document explores the concept of orthogonal trajectories and their derivation for various curve families. The content is presented with mathematical rigor, including formulas, derivations, and example solutions.

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Module 3

Ordinary differential equations of first order
3.1 Linear and Bernoulli’s differential equations

Introduction:

1. Linear differential equation in 𝒚:
𝑑𝑦
This is of the form 𝑑𝑥 + 𝑃𝑦 = 𝑄, where 𝑃 and 𝑄 are functions of 𝑥 alone.

General solution is 𝑦. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑥 + 𝑐, where 𝐼𝐹 = 𝑒 ∫ 𝑃𝑑𝑥 .

2. Linear differential equation in 𝒙:
𝑑𝑥
This is of the form + 𝑃𝑥 = 𝑄, where 𝑃 and 𝑄 are functions of 𝑦 alone.
𝑑𝑦

General solution is 𝑥. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑦 + 𝑐, where 𝐼𝐹 = 𝑒 ∫ 𝑃𝑑𝑦 .

3. Bernoulli’s differential equation in 𝒚:
𝑑𝑦
This is of the form 𝑑𝑥 + 𝑃𝑦 = 𝑄𝑦 𝑛 , where 𝑃 and 𝑄 are functions of 𝑥 alone.
𝑑𝑦
Dividing this equation by 𝑦 𝑛 , 𝑦 −𝑛 + 𝑃𝑦 1−𝑛 = 𝑄 ---- (1)
𝑑𝑥

𝑑𝑦 𝑑𝑡
Put 𝑦1−𝑛 = 𝑡, then (1 − 𝑛)𝑦 −𝑛 = 𝑑𝑥
𝑑𝑥

1 𝑑𝑡
Equation (1) becomes 1−𝑛 + 𝑃𝑡 = 𝑄
𝑑𝑥

𝑑𝑡
Reduced linear differential equation is 𝑑𝑥 + (1 − 𝑛)𝑃𝑡 = (1 − 𝑛)𝑄

4. Bernoulli’s differential equation in 𝒙:
𝑑𝑦
This is of the form 𝑑𝑥 + 𝑃𝑥 = 𝑄𝑥 𝑛 , where 𝑃 and 𝑄 are functions of 𝑦 alone.
𝑑𝑦
Dividing this equation by 𝑥 𝑛 , 𝑥 −𝑛 + 𝑃𝑥1−𝑛 = 𝑄 ---- (1)
𝑑𝑥

𝑑𝑥 𝑑𝑡
Put 𝑥1−𝑛 = 𝑡, then (1 − 𝑛)𝑥 −𝑛 = 𝑑𝑦
𝑑𝑦

1 𝑑𝑡
Equation (1) becomes 1−𝑛 + 𝑃𝑡 = 𝑄
𝑑𝑦

𝑑𝑡
Reduced linear differential equation is 𝑑𝑦 + (1 − 𝑛)𝑃𝑡 = (1 − 𝑛)𝑄




Dr. Narasimhan G, RNSIT 1

,Problems:

𝒅𝒚
1. Solve 𝒅𝒙 + 𝒚 𝒄𝒐𝒕 𝒙 = 𝒄𝒐𝒔 𝒙

This is a linear L.D.E in 𝑦 with 𝑃 = cot 𝑥 , 𝑄 = cos 𝑥
𝐼𝐹 = 𝑒 ∫ 𝑃𝑑𝑥 = 𝑒 ∫ cot 𝑥𝑑𝑥 = sin 𝑥
General solution is 𝑦. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑥 + 𝑐
𝑦. sin 𝑥 = ∫ cos 𝑥 . sin 𝑥 𝑑𝑥 + 𝑐
1
𝑦 sin 𝑥 = 2 ∫ sin 2𝑥 𝑑𝑥 + 𝑐
1
𝑦 sin 𝑥 = − 4 cos 2𝑥 + 𝑐


𝒅𝒚
2. Solve 𝒅𝒙 + 𝒚 𝒕𝒂𝒏 𝒙 = 𝒚𝟑 𝒔𝒆𝒄 𝒙

Step 1: Reduce it to an LDE
Divide by 𝑦 3 on both sides,
1 𝑑𝑦 1
+ 𝑦 2 tan 𝑥 = sec 𝑥 ---- (1)
𝑦 3 𝑑𝑥
1 2 𝑑𝑦 𝑑𝑡
If 𝑦 2 = 𝑡 then − 𝑦 3 𝑑𝑥 = 𝑑𝑥
1 1 𝑑𝑦 1 𝑑𝑡
Put 𝑦 2 = 𝑡, = − 2 𝑑𝑥 in (1)
𝑦 3 𝑑𝑥
1 𝑑𝑡
− 2 𝑑𝑥 + 𝑡 tan 𝑥 = sec 𝑥

Multiply by -2 on both sides,
𝑑𝑡
− 2𝑡 tan 𝑥 = −2 sec 𝑥
𝑑𝑥

This is an LDE in 𝑡 with 𝑃 = −2 tan 𝑥 , 𝑄 = −2 sec 𝑥
Step 2: Solve reduced LDE
𝐼𝐹 = 𝑒 ∫ −2 tan 𝑥𝑑𝑥 = 𝑒 −2 log sec 𝑥 = cos 2 𝑥
General solution is 𝑡. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑥 + 𝑐
𝑡 cos2 𝑥 = ∫ −2 sec 𝑥 cos2 𝑥 𝑑𝑥 + 𝑐
𝑡 cos2 𝑥 = −2 sin 𝑥 + 𝑐
1
(𝑦 2 ) cos 2 𝑥 = −2 sin 𝑥 + 𝑐




Dr. Narasimhan G, RNSIT 2

, 𝒅𝒚 𝒚
3. Solve + = 𝒚𝟐 𝒙 (May 22)
𝒅𝒙 𝒙


Step 1: Reduce it to an LDE

Divide by 𝑦 2 on both sides,

1 𝑑𝑦 1 1
+ 𝑥 (𝑦) = 𝑥 ---- (1)
𝑦 2 𝑑𝑥

1 1 𝑑𝑦 𝑑𝑡
If 𝑦 = 𝑡 then − 𝑦 2 𝑑𝑥 = 𝑑𝑥

1 1 𝑑𝑦 𝑑𝑡
Put 𝑦 = 𝑡, = − 𝑑𝑥 in (1)
𝑦2 𝑑𝑥

𝑑𝑡 𝑡
− 𝑑𝑥 + 𝑥 = 𝑥

Multiply by -1 on both sides,

𝑑𝑡 𝑡
− 𝑥 = −𝑥
𝑑𝑥


This is an LDE in 𝑡 with 𝑃 = −1/𝑥, 𝑄 = −𝑥

Step 2: Solve reduced LDE
1
1
𝐼𝐹 = 𝑒 ∫ −𝑥 𝑑𝑥 = 𝑒 − log 𝑥 = 𝑥

General solution is 𝑡. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑥 + 𝑐

1 1
𝑡 𝑥 = ∫ − 𝑥 𝑥 𝑑𝑥 + 𝑐

1
𝑡 𝑥 = −𝑥 + 𝑐

1
= −𝑥 + 𝑐
𝑥𝑦




Dr. Narasimhan G, RNSIT 3

, 𝒅𝒚
4. 𝒕𝒂𝒏 𝒚 + 𝒕𝒂𝒏 𝒙 = 𝒄𝒐𝒔 𝒚 𝒄𝒐𝒔𝟐 𝒙
𝒅𝒙


Step 1: Reduce it to an LDE

Divide by cos 𝑦 on both sides,

𝑑𝑦
sec 𝑦 tan 𝑦 𝑑𝑥 + sec 𝑦 tan 𝑥 = cos 2 𝑥 ---- (1)

𝑑𝑦 𝑑𝑡
If sec 𝑦 = 𝑡 then sec 𝑦 tan 𝑦 𝑑𝑥 = 𝑑𝑥

𝑑𝑡
(1) ⇒ 𝑑𝑥 + 𝑡 tan 𝑥 = cos2 𝑥

This is an LDE in 𝑡 with 𝑃 = tan 𝑥 , 𝑄 = cos 2 𝑥

Step 2: Solve reduced LDE

𝐼𝐹 = 𝑒 ∫ 𝑃 𝑑𝑥 = 𝑒 ∫ tan 𝑥 𝑑𝑥 = sec 𝑥

General solution is 𝑡. 𝐼𝐹 = ∫ 𝑄. 𝐼𝐹 𝑑𝑥 + 𝑐

𝑡 sec 𝑥 = ∫ cos 2 𝑥 sec 𝑥 𝑑𝑥 + 𝑐

sec 𝑦 sec 𝑥 = sin 𝑥 + 𝑐




Dr. Narasimhan G, RNSIT 4

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