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DIFFERENTIAL EQUATION (MT-202) SYED AZEEM INAM
DIFFERENTIAL EQUATION (MT-202)
LECTURE #11
HIGHER ORDER DIFFERENTIAL EQUATIONS:
NON-HOMOGENOUS LINEAR DIFFERENTIAL EQUATIONS:
The equations
𝑎0
𝑑 𝑛
𝑦
𝑑𝑥 𝑛
+ 𝑎1
𝑑 𝑛−1
𝑦
𝑑𝑥 𝑛−1
+ ⋯ + 𝑎 𝑛−1
𝑑𝑦
𝑑𝑥
+ 𝑎 𝑛 𝑦 = 𝐹(𝑥)
Where 𝑎0, 𝑎1, … , 𝑎 𝑛−1, 𝑎 𝑛 are real constants is called the higher order non-
homogenous differential equation and its general solution is compose to two parts.
i.e.
General solution = Complimentary solution + Particular Solution
RULES TO FIND PARTICULAR INTEGRAL:
RULE 1:
1
𝑓(𝐷)
𝑒 𝑎𝑥
=
1
𝑓(𝑎)
𝑒 𝑎𝑥
If 𝑓(𝑎) = 0 then
1
𝑓(𝐷)
𝑒 𝑎𝑥
= 𝑥
1
𝑓′(𝑎)
𝑒 𝑎𝑥
If 𝑓′′(𝑎) = 0 then
1
𝑓(𝐷)
𝑒 𝑎𝑥
= 𝑥2
1
𝑓′′(𝑎)
𝑒 𝑎𝑥
And so on.
RULE 2:
1
𝑓(𝐷)
𝑠𝑖𝑛𝑎𝑥 =
1
𝑓(−𝑎2)
𝑠𝑖𝑛𝑎𝑥
If 𝑓(−𝑎2) = 0 then
DIFFERENTIAL EQUATION (MT-202) SYED AZEEM INAM
DIFFERENTIAL EQUATION (MT-202)
1
𝑓(𝐷)
𝑠𝑖𝑛𝑎𝑥 = 𝑥
1
𝑓′(−𝑎2)
𝑠𝑖𝑛𝑎𝑥
If 𝑓′(−𝑎2) = 0 then
1
𝑓(𝐷)
𝑠𝑖𝑛𝑎𝑥 = 𝑥2
1
𝑓′′(−𝑎2)
𝑠𝑖𝑛𝑎𝑥
And so on.
Similarly,
1
𝑓(𝐷)
𝑐𝑜𝑠𝑎𝑥 =
1
𝑓(−𝑎2)
𝑐𝑜𝑠𝑎𝑥
If 𝑓(−𝑎2) = 0 then
1
𝑓(𝐷)
𝑐𝑜𝑠𝑎𝑥 = 𝑥
1
𝑓′(−𝑎2)
𝑐𝑜𝑠𝑎𝑥
If 𝑓′(−𝑎2) = 0 then
1
𝑓(𝐷)
𝑐𝑜𝑠𝑎𝑥 = 𝑥2
1
𝑓′′(−𝑎2)
𝑐𝑜𝑠𝑎𝑥
And so on.

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differential equation Lecture#11

  • 1. DIFFERENTIAL EQUATION (MT-202) SYED AZEEM INAM DIFFERENTIAL EQUATION (MT-202) LECTURE #11 HIGHER ORDER DIFFERENTIAL EQUATIONS: NON-HOMOGENOUS LINEAR DIFFERENTIAL EQUATIONS: The equations 𝑎0 𝑑 𝑛 𝑦 𝑑𝑥 𝑛 + 𝑎1 𝑑 𝑛−1 𝑦 𝑑𝑥 𝑛−1 + ⋯ + 𝑎 𝑛−1 𝑑𝑦 𝑑𝑥 + 𝑎 𝑛 𝑦 = 𝐹(𝑥) Where 𝑎0, 𝑎1, … , 𝑎 𝑛−1, 𝑎 𝑛 are real constants is called the higher order non- homogenous differential equation and its general solution is compose to two parts. i.e. General solution = Complimentary solution + Particular Solution RULES TO FIND PARTICULAR INTEGRAL: RULE 1: 1 𝑓(𝐷) 𝑒 𝑎𝑥 = 1 𝑓(𝑎) 𝑒 𝑎𝑥 If 𝑓(𝑎) = 0 then 1 𝑓(𝐷) 𝑒 𝑎𝑥 = 𝑥 1 𝑓′(𝑎) 𝑒 𝑎𝑥 If 𝑓′′(𝑎) = 0 then 1 𝑓(𝐷) 𝑒 𝑎𝑥 = 𝑥2 1 𝑓′′(𝑎) 𝑒 𝑎𝑥 And so on. RULE 2: 1 𝑓(𝐷) 𝑠𝑖𝑛𝑎𝑥 = 1 𝑓(−𝑎2) 𝑠𝑖𝑛𝑎𝑥 If 𝑓(−𝑎2) = 0 then
  • 2. DIFFERENTIAL EQUATION (MT-202) SYED AZEEM INAM DIFFERENTIAL EQUATION (MT-202) 1 𝑓(𝐷) 𝑠𝑖𝑛𝑎𝑥 = 𝑥 1 𝑓′(−𝑎2) 𝑠𝑖𝑛𝑎𝑥 If 𝑓′(−𝑎2) = 0 then 1 𝑓(𝐷) 𝑠𝑖𝑛𝑎𝑥 = 𝑥2 1 𝑓′′(−𝑎2) 𝑠𝑖𝑛𝑎𝑥 And so on. Similarly, 1 𝑓(𝐷) 𝑐𝑜𝑠𝑎𝑥 = 1 𝑓(−𝑎2) 𝑐𝑜𝑠𝑎𝑥 If 𝑓(−𝑎2) = 0 then 1 𝑓(𝐷) 𝑐𝑜𝑠𝑎𝑥 = 𝑥 1 𝑓′(−𝑎2) 𝑐𝑜𝑠𝑎𝑥 If 𝑓′(−𝑎2) = 0 then 1 𝑓(𝐷) 𝑐𝑜𝑠𝑎𝑥 = 𝑥2 1 𝑓′′(−𝑎2) 𝑐𝑜𝑠𝑎𝑥 And so on.