5.5.5 Example E Assume that c = 0 in equation (5.183) and continue to assume that F(k,l) is a solution to the homogeneous equation. Under these conditions, we have (aE1 + bE2)z(k, l) = F(k, l) (5.189) and (aE1 + bE2)F(k, l) = 0. (5.190) The solution to the last equation is F(k, €) = (-b/a)* f(e+ k), (5.191) where f is an arbitrary function of l + k. Examination of the left-hand side of equation (5.189) shows that it is of a form such that Laplace's method can be used to obtain a solution. If we let k +l = m = constant, Vk = z(k, l) = z(k, m – k), (5.192) then vk satisfies the first-order inhomogeneous equation avk+1 + bvk = (-b/a)*f(m), (5.193) where we have used the results of equations (5.191) and (5.192) to replace the right-hand side of equation (5.189). Note that f(m) is a constant. Solving for Vk gives k k - f(m)k (5.194) Vk = A | a where A is an arbitrary constant. Replacing m by l+k and A by an arbitrary function of l + k gives the complete solution to equation (5.189), under the assumption of equation (5.190),

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Chapter2: Second-order Linear Odes
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Explain the determine blue

5.5.5 Example E
Assume that c = 0 in equation (5.183) and continue to assume that F(k,l) is
a solution to the homogeneous equation. Under these conditions, we have
(aE1 + bE2)z(k, e) = F(k, l)
(5.189)
and
(aE1 + bE2)F(k, l) = 0.
(5.190)
The solution to the last equation is
F(k, €) = (-b/a)* f(l+ k),
(5.191)
where f is an arbitrary function of l + k.
Examination of the left-hand side of equ
form such that Laplace's method can be used to obtain a solution. If we let
on (5.189) shows that it is of a
k + l = m = constant,
Vk =
z(k, l)
= z(k, m – k),
(5.192)
then vk satisfies the first-order inhomogeneous equation
avk+1 + bvk = (-6/a)kƒ(m),
(5.193)
where we have used the results of equations (5.191) and (5.192) to replace the
right-hand side of equation (5.189). Note that f(m) is a constant. Solving for
Vk gives
k
k
Uk = A
(5.194)
a
where A is an arbitrary constant. Replacing m by l+k and A by an arbitrary
function of l +k_gives the complete solution to equation (5.189), under the
assumption of equation (5.190),
k
k
k
z (k, €) = (-2) g(e+ k) –
f(l + k).
(5.195)
-
a
a
Transcribed Image Text:5.5.5 Example E Assume that c = 0 in equation (5.183) and continue to assume that F(k,l) is a solution to the homogeneous equation. Under these conditions, we have (aE1 + bE2)z(k, e) = F(k, l) (5.189) and (aE1 + bE2)F(k, l) = 0. (5.190) The solution to the last equation is F(k, €) = (-b/a)* f(l+ k), (5.191) where f is an arbitrary function of l + k. Examination of the left-hand side of equ form such that Laplace's method can be used to obtain a solution. If we let on (5.189) shows that it is of a k + l = m = constant, Vk = z(k, l) = z(k, m – k), (5.192) then vk satisfies the first-order inhomogeneous equation avk+1 + bvk = (-6/a)kƒ(m), (5.193) where we have used the results of equations (5.191) and (5.192) to replace the right-hand side of equation (5.189). Note that f(m) is a constant. Solving for Vk gives k k Uk = A (5.194) a where A is an arbitrary constant. Replacing m by l+k and A by an arbitrary function of l +k_gives the complete solution to equation (5.189), under the assumption of equation (5.190), k k k z (k, €) = (-2) g(e+ k) – f(l + k). (5.195) - a a
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