Method of Variation of ParametersBy Kaushal Patel
Method of Variation of Parameters
βΊ Langrage invented the method of variation of parameters.
βΊ Consider differential equation of the form f(D)y=X.
βΊ when X is of the form πππ₯ , sin ππ₯, cos ππ₯, π₯π, πππ₯ . π£ or any function of x, then the shortcut methods are available which will discuss later on. If X be of any other form say tan π₯, sec π₯ , csc π₯ ππ‘π. , then we have to use one of the following methods.
I. The method of partial fractions
II. The method of variation of parameters
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βΊ Consider the second order linear differential equation with constant co-efficient
π2π¦
ππ₯2+ π1
ππ¦
ππ₯+ π2π¦ = π β¦β¦(i)
βΊ Let the complementary function of (i) be π¦ = π1π¦1 + π2π¦2
βΊ Then π¦1 and π¦2 satisfy the equation
π2π¦
ππ₯2+ π1
ππ¦
ππ₯+ π2π¦ = 0 β¦β¦(ii)
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βΊ Let us assume that the particular integral of (i) be
π¦ = π’π¦1 + π£π¦2 β¦β¦(iii)
where u and v are unknown functions of x
βΊ Differentiating w.r. to x, we have
π¦β² = π’π¦1β² + π’β²π¦1 + π£π¦2
β² + π£β²π¦2 β¦β¦(iv)
βΊ To determine two unknown functions u and v, we need two equations.
We assume that π’β²π¦1 + π£β²π¦2 = 0 β¦β¦(v)
β΄(iv) reduces to
π¦β² = π’π¦1β² + π£π¦2
β² β¦β¦(vi)
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βΊ Differentiating w.r. to x, we getπ¦" = π’π¦1
" + π’β²π¦1β² + π£π¦2
" + π£β²π¦2β²
βΊ Substituting the values of π¦, π¦β² and π¦" in (i), we have
π’ π¦1" + π1π¦1
β² + π2π¦1 + π£ π¦2" + π1π¦2
β² + π2π¦2 + π’β²π¦1β² + π£β²π¦2
β² = π β¦β¦(vii)
βΊ But π¦1 and π¦2 satisfy equation (ii)
β΄ π¦1" + π1π¦1
β² + π2π¦1 = 0 and π¦2" + π1π¦2
β² + π2π¦2 = 0
βΊ Equation (viii) takes the form,
π’β²π¦1β² + π£β²π¦2
β² = π β¦β¦(viii)
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βΊ Solving (v) and (ix), we get
π’β² =π¦2π
π¦1π¦2β²βπ¦2π¦1
β² and π£β² =π¦1π
π¦1π¦2β²βπ¦2π¦1
β²
βΊ Integrating, we get
π’ = β π¦2π
π€ππ₯ and v = β
π¦1π
π€ππ₯, where π€ = π¦1π¦2
β² β π¦2π¦1β²
βΊ Substituting the values of u and v in (iii), we have
π. πΌ = π¦ = βπ¦1 π¦2π
π€ππ₯+π¦2
π¦1π
π€ππ₯ β¦β¦(ix)
Example
Find general solution of π¦" + 9π¦ = sec 3π₯ by method of variation of parameters.
Solution:-
βΊ The given differential equation can be written as,
π·2 + 9 π¦ = sec 3π₯ , π€βπππ π· =π
ππ₯
βΊ The auxiliary equation is,π·2 + 9 = 0
=>π· = Β±3π
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βΊ Hence, complimentary function isπ¦π = π1 cos 3π₯ + π2 sin 3π₯
βΊ Now we take π¦1 = cos 3π₯ , π¦2 = sin 3π₯
π€ =π¦1 π¦2π¦1β² π¦2
β² =cos 3π₯ sin 3π₯β3 sin 3π₯ 3 cos 3π₯
=3
βΊ Particular integral is,
π¦π = βπ¦1 π¦2π
π€ππ₯ + π¦2
π¦1π
π€ππ₯
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= βcos 3π₯ sin 3π₯ sec 3π₯
3ππ₯ + sin 3π₯
cos 3π₯ sec 3π₯
3ππ₯
= βcos 3π₯
3 tan3π₯ ππ₯ +
sin 3π₯
3 ππ₯
=cos 3π₯ log(cos 3π₯)
9+π₯ sin 3π₯
3
βΊ Hence, general solution is
y(x)= π¦π + π¦π
= π1 cos 3π₯ + π2 sin 3π₯ +cos 3π₯ log(cos 3π₯)
9+π₯ sin 3π₯
3
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