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π‘Ž0 π‘₯
𝑛
𝑑 𝑛 𝑦
𝑑π‘₯ 𝑛
+ π‘Ž. π‘₯ π‘›βˆ’1
𝑑 π‘›βˆ’1𝑦
π‘‘π‘›βˆ’1
+ β‹― + π‘Ž π‘›βˆ’1 π‘₯
𝑑𝑦
𝑑π‘₯
+ π‘Ž 𝑛 𝑦 = 𝑓(π‘₯)
CAUCHY-EULAR DIFFRENTIAL EQUATION
Cauchy–Euler equation s a linear homogeneous ordinary differential
equation with variable coefficients. It is sometimes referred to as
an equidimensional equation. Because of its particularly simple equidimensional
structure the differential equation can be solved explicitly.
π‘Ž0 π‘₯
𝑛
𝑑 𝑛 𝑦
𝑑π‘₯ 𝑛
+ π‘Ž. π‘₯ π‘›βˆ’1
𝑑 π‘›βˆ’1𝑦
π‘‘π‘›βˆ’1
+ β‹― + π‘Ž π‘›βˆ’1 π‘₯
𝑑𝑦
𝑑π‘₯
+ π‘Ž 𝑛 𝑦 = 𝑓(π‘₯)
π‘Ž0 π‘₯
𝑛
𝑑 𝑛 𝑦
𝑑π‘₯ 𝑛
+ π‘Ž. π‘₯ π‘›βˆ’1
𝑑 π‘›βˆ’1𝑦
π‘‘π‘›βˆ’1
+ β‹― + π‘Ž π‘›βˆ’1 π‘₯
𝑑𝑦
𝑑π‘₯
+ π‘Ž 𝑛 𝑦 = 𝑓(π‘₯)
β€’ This equation is called Cauchy Euler equation
β€’ We can convert this equation into linear
β€’ equation by substituting x= 𝒆 𝒕
= 𝒍𝒏𝒙 = 𝒕
β€’
1
π‘₯
=
𝑑𝑑
𝑑π‘₯
β€’
𝑑𝑦
𝑑π‘₯
=
𝑑𝑦
𝑑𝑑
.
𝑑𝑑
𝑑π‘₯
=
𝑑𝑦
𝑑𝑑
.
1
π‘₯
β€’ =>
π‘₯𝑑𝑦
𝑑π‘₯
=
𝑑𝑦
𝑑𝑑
= βˆ†π‘¦
π‘Ž0 π‘₯
𝑛
𝑑 𝑛 𝑦
𝑑π‘₯ 𝑛
+ π‘Ž. π‘₯ π‘›βˆ’1
𝑑 π‘›βˆ’1𝑦
π‘‘π‘›βˆ’1
+ β‹― + π‘Ž π‘›βˆ’1 π‘₯
𝑑𝑦
𝑑π‘₯
+ π‘Ž 𝑛 𝑦 = 𝑓(π‘₯)
β€’
𝑑𝑦
𝑑π‘₯
=
1
π‘₯
𝑑𝑦
𝑑𝑑
β€’
𝑑2 𝑦
𝑑π‘₯2 =
1
π‘₯
𝑑2
𝑑𝑑2 .
𝑑𝑑
𝑑π‘₯
+
𝑑𝑦
𝑑𝑑
βˆ’1
π‘₯2
β€’
𝑑2 𝑦
𝑑π‘₯2 =
1
π‘₯
𝑑2
𝑑𝑑2 .
1
π‘₯
βˆ’
𝑑𝑦
𝑑𝑑
1
π‘₯2
β€’
𝑑2 𝑦
𝑑π‘₯2 =
1
π‘₯2 (
𝑑2 𝑦
𝑑π‘₯2 βˆ’
𝑑𝑦
𝑑𝑑
)
π‘₯2 𝑑𝑦
𝑑π‘₯2 = ( βˆ†2 βˆ’ βˆ†)𝑦
οƒžβˆ† βˆ† βˆ’ 1 𝑦
οƒž
π‘₯3𝑑3
𝑦
𝑑π‘₯3 =
οƒžβˆ† βˆ† βˆ’ 1 (βˆ† βˆ’
PROBLEM:
π‘₯2
𝑑2 𝑦
𝑑π‘₯2
+ 7π‘₯
𝑑𝑦
𝑑π‘₯
+ 5𝑦 = π‘₯5
Solution: x= 𝑒 𝑑
β‡’ 𝑙𝑛π‘₯ = 𝑑
So,
𝑑𝑑
𝑑π‘₯
=
1
π‘₯
Now we know the values already, therefore,
π‘₯2 𝑑2 𝑦
𝑑π‘₯2 =βˆ† βˆ† βˆ’ 1 𝑦
π‘₯
𝑑𝑦
𝑑π‘₯
= βˆ†βˆ†π‘¦ βˆ†
β‡’ βˆ†(βˆ† βˆ’ 1)𝑦 + 7 βˆ†π‘¦ + 5𝑦 = 𝑒5𝑑
β‡’ (βˆ†2 βˆ’βˆ† + 7βˆ† + 5)𝑦 = 𝑒5π‘₯
οƒž(βˆ†2= 6βˆ† + 5 )𝑦 = 𝑒5π‘₯
Remaining Problem

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Cauchy Eular Differential Equation

  • 1. π‘Ž0 π‘₯ 𝑛 𝑑 𝑛 𝑦 𝑑π‘₯ 𝑛 + π‘Ž. π‘₯ π‘›βˆ’1 𝑑 π‘›βˆ’1𝑦 π‘‘π‘›βˆ’1 + β‹― + π‘Ž π‘›βˆ’1 π‘₯ 𝑑𝑦 𝑑π‘₯ + π‘Ž 𝑛 𝑦 = 𝑓(π‘₯) CAUCHY-EULAR DIFFRENTIAL EQUATION Cauchy–Euler equation s a linear homogeneous ordinary differential equation with variable coefficients. It is sometimes referred to as an equidimensional equation. Because of its particularly simple equidimensional structure the differential equation can be solved explicitly.
  • 2. π‘Ž0 π‘₯ 𝑛 𝑑 𝑛 𝑦 𝑑π‘₯ 𝑛 + π‘Ž. π‘₯ π‘›βˆ’1 𝑑 π‘›βˆ’1𝑦 π‘‘π‘›βˆ’1 + β‹― + π‘Ž π‘›βˆ’1 π‘₯ 𝑑𝑦 𝑑π‘₯ + π‘Ž 𝑛 𝑦 = 𝑓(π‘₯) π‘Ž0 π‘₯ 𝑛 𝑑 𝑛 𝑦 𝑑π‘₯ 𝑛 + π‘Ž. π‘₯ π‘›βˆ’1 𝑑 π‘›βˆ’1𝑦 π‘‘π‘›βˆ’1 + β‹― + π‘Ž π‘›βˆ’1 π‘₯ 𝑑𝑦 𝑑π‘₯ + π‘Ž 𝑛 𝑦 = 𝑓(π‘₯) β€’ This equation is called Cauchy Euler equation β€’ We can convert this equation into linear β€’ equation by substituting x= 𝒆 𝒕 = 𝒍𝒏𝒙 = 𝒕 β€’ 1 π‘₯ = 𝑑𝑑 𝑑π‘₯ β€’ 𝑑𝑦 𝑑π‘₯ = 𝑑𝑦 𝑑𝑑 . 𝑑𝑑 𝑑π‘₯ = 𝑑𝑦 𝑑𝑑 . 1 π‘₯ β€’ => π‘₯𝑑𝑦 𝑑π‘₯ = 𝑑𝑦 𝑑𝑑 = βˆ†π‘¦ π‘Ž0 π‘₯ 𝑛 𝑑 𝑛 𝑦 𝑑π‘₯ 𝑛 + π‘Ž. π‘₯ π‘›βˆ’1 𝑑 π‘›βˆ’1𝑦 π‘‘π‘›βˆ’1 + β‹― + π‘Ž π‘›βˆ’1 π‘₯ 𝑑𝑦 𝑑π‘₯ + π‘Ž 𝑛 𝑦 = 𝑓(π‘₯)
  • 3. β€’ 𝑑𝑦 𝑑π‘₯ = 1 π‘₯ 𝑑𝑦 𝑑𝑑 β€’ 𝑑2 𝑦 𝑑π‘₯2 = 1 π‘₯ 𝑑2 𝑑𝑑2 . 𝑑𝑑 𝑑π‘₯ + 𝑑𝑦 𝑑𝑑 βˆ’1 π‘₯2 β€’ 𝑑2 𝑦 𝑑π‘₯2 = 1 π‘₯ 𝑑2 𝑑𝑑2 . 1 π‘₯ βˆ’ 𝑑𝑦 𝑑𝑑 1 π‘₯2 β€’ 𝑑2 𝑦 𝑑π‘₯2 = 1 π‘₯2 ( 𝑑2 𝑦 𝑑π‘₯2 βˆ’ 𝑑𝑦 𝑑𝑑 ) π‘₯2 𝑑𝑦 𝑑π‘₯2 = ( βˆ†2 βˆ’ βˆ†)𝑦 οƒžβˆ† βˆ† βˆ’ 1 𝑦 οƒž π‘₯3𝑑3 𝑦 𝑑π‘₯3 = οƒžβˆ† βˆ† βˆ’ 1 (βˆ† βˆ’
  • 4. PROBLEM: π‘₯2 𝑑2 𝑦 𝑑π‘₯2 + 7π‘₯ 𝑑𝑦 𝑑π‘₯ + 5𝑦 = π‘₯5 Solution: x= 𝑒 𝑑 β‡’ 𝑙𝑛π‘₯ = 𝑑 So, 𝑑𝑑 𝑑π‘₯ = 1 π‘₯ Now we know the values already, therefore, π‘₯2 𝑑2 𝑦 𝑑π‘₯2 =βˆ† βˆ† βˆ’ 1 𝑦 π‘₯ 𝑑𝑦 𝑑π‘₯ = βˆ†βˆ†π‘¦ βˆ†
  • 5. β‡’ βˆ†(βˆ† βˆ’ 1)𝑦 + 7 βˆ†π‘¦ + 5𝑦 = 𝑒5𝑑 β‡’ (βˆ†2 βˆ’βˆ† + 7βˆ† + 5)𝑦 = 𝑒5π‘₯ οƒž(βˆ†2= 6βˆ† + 5 )𝑦 = 𝑒5π‘₯