1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

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22 Chapter 0 Ordinary Differential Equations


Thus, we are left with a pair of simultaneous equations,
v′ 1 u 1 +v′ 2 u 2 =0, (12′)

v′ 1 u′ 1 +v′ 2 u′ 2 =f(t), (15)

in the unknownsv′ 1 andv′ 2. The determinant of this system is
∣∣
∣∣


u 1 u 2
u′ 1 u′ 2

∣∣

∣∣

∣=W(t), (16)

the Wronskian ofu 1 andu 2. Since these were to be independent solutions of
Eq. (10), their Wronskian is nonzero, and we may solve forv′ 1 (t)andv′ 2 (t)and
hence forv 1 andv 2.


Example.
Use variation of parameters to solve the nonhomogeneous equation


d^2 u
dt^2

+u=cos(ωt).

Assume a solution in the form


up(t)=v 1 cos(t)+v 2 sin(t),

because sin(t)and cos(t)are independent solutions of the corresponding ho-
mogeneous equationu′′+u=0. The assumption of Eq. (12) is


v 1 ′cos(t)+v′ 2 sin(t)= 0. (17)

Then our equation reduces to the following, corresponding to Eq. (15):


−v 1 ′sin(t)+v 2 ′cos(t)=cos(ωt). (18)

Now we solve Eqs. (17) and (18) simultaneously to find


v 1 ′=−sin(t)cos(ωt), v′ 2 =cos(t)cos(ωt). (19)

Theseequationsaretobeintegratedtofindv 1 andv 2 ,andthenup(t). 


Finally, we note thatv 1 (t)andv 2 (t)can be found from Eqs. (12) and (15)
in general:


v 1 ′=−u^2 f
W

,v′ 2 =u^1 f
W

. (20)

Integrating these two equations, we find that


v 1 (t)=−

∫ u
2 (t)f(t)
W(t)

dt,v 2 (t)=

∫ u
1 (t)f(t)
W(t)

dt. (21)
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