(1.2) Initial-Value Problems
INTRODUCTION:
We are often interested in problems in which we seek a solution π¦(π₯) of a differential equation so that
π¦(π₯) satisfies prescribed side conditionsβthat is, conditions imposed on the unknown π¦(π₯) or its
derivatives. On some interval πΌ containing π₯0 the problem
ππππ£π:
ππ π¦
= π(π₯, π¦, π¦ β² , β¦ , π¦ (πβ1) )
ππ₯ π
ππ’πππππ‘ π‘π:
π¦(π₯0 ) = π¦0 , π¦ β² (π₯0 ) = π¦1 , β¦ , π¦ (πβ1) (π₯0 ) = π¦πβ1 ,
β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ (1)
where π¦0 , π¦1 , β¦ , π¦πβ1 are arbitrarily specified real constants, is called an initial-value problem
(IVP). The values of π¦(π₯) and its first π β 1 derivatives at a single point π₯0 , π¦(π₯0 ) = π¦0 , π¦ β² (π₯0 ) =
π¦1 , β¦ , π¦ (πβ1) (π₯0 ) = π¦πβ1 , are called initial conditions.
FIRST- AND SECOND-ORDER IVPS:
The problem given in (1) is also called an πth-order initial-value problem. For example,
ππππ£π:
ππ’πππππ‘ π‘π:
and
ππππ£π:
ππ’πππππ‘ π‘π:
ππ¦
= π (π₯, π¦)
ππ₯
β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ (2)
π¦(π₯0 ) = π¦0
π2 π¦
= π (π₯, π¦, π¦ β² )
2
ππ₯
π¦(π₯0 ) = π¦0 , π¦ β² (π₯0 ) = π¦1
β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ (3)
are first- and second-order initial-value problems, respectively.
THEOREM 1.2.1 (Existence of a Unique Solution)
Let π
be a rectangular region in the π₯π¦-plane defined by π β€ π₯ β€ π, π β€ π¦ β€ π that contains the
point (π₯0 , π¦0 ) in its interior. If π (π₯, π¦) and ππ βππ¦ are continuous on π
, then there exists some interval
πΌ0 : (π₯0 β β, π₯0 + β), β > 0, contained in [π, π], and a unique function π¦(π₯), defined on πΌ0 , that is a
solution of the initial-value problem (2).
ππ¦
Roughly speaking, if we have the IVP
= π (π₯, π¦), π¦(π₯0 ) = π¦0 , then we have 3 cases explain the
ππ₯
theorem which are follows:
ο· If π (π₯, π¦) and ππ/ππ¦ are continuous on a common domain πΌ
β the solution of the IVP exists and unique.
ο· If π (π₯, π¦) is only continuous on a domain πΌ
β the solution of the IVP exists only. This means that the IVP has infinite solutions
ο· If π (π₯, π¦) is discontinuous on a domain πΌ
β the solution of the IVP does not exist.
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(1.2) Initial-Value Problems
EXAMPLE 1 (Second-Order IVP)
In Example 4 of Section 1.1, we saw that
π₯ = π1 cos 4π‘ + π2 sin 4π‘
is a two-parameter family of solutions of
π₯ β²β² + 16π₯ = 0.
Find a solution of the initial-value problem
π
π
π₯ β²β² + 16π₯ = 0, π₯ ( ) = β2, π₯ β² ( ) = 1.
2
2
β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ β¦ (4)
SOLUTION:
We first find π₯ β² and π₯ β²β² using the general solution π₯ = π1 cos 4π‘ + π2 sin 4π‘ , we obtain
π₯ β² = β4π1 sin 4π‘ + 4π2 cos 4π‘
and
π
π₯ β²β² = β16π1 cos 4π‘ β 16π2 sin 4π‘.
Then, we apply π₯ ( ) = β2 to the given family of solutions:
2
π
π
π
π₯ ( ) = π1 cos (4 ( )) + π2 sin (4 ( )) = π1 cos 2π + π2 sin 2π = π1 (1) + π2 (0) = π1 = β2.
2
2
2
π
Hence, π1 = β2. Similarly, we next apply π₯ β² ( ) = 1 to the two-parameter family
2
π₯ β² = β4π1 sin 4π‘ + 4π2 cos 4π‘.
So,
π
π
π
π₯ β² ( ) = β4(β2) sin (4 ( )) + 4π2 cos (4 ( )) = 8 sin 2π + 4π2 cos 2π = 8(0) + 4π2 (1) = 4π2 = 1.
2
2
2
1
Thus, π2 = . Hence,
4
1
π₯ = β2 cos 4π‘ + sin 4π‘
4
is a solution of (4).
EXAMPLE 2
According to the Existence and Uniqueness Theorem, determine whether the IVP
has a unique solution.
SOLUTION:
ππ¦
= π₯π¦1/2 ,
ππ₯
π¦ (0) = 0
1
1 β π(π₯, π¦) = π₯π¦ 2 = π₯ βπ¦ is continuous on {(π₯, π¦): π₯ β β and π¦ β [0, β)}.
ππ
π₯
π₯
2β
= 1=
is continuous on {(π₯, π¦): π₯ β β and π¦ β (0, β)}.
ππ¦ 2π¦ 2 2βπ¦
Since (0,0) is not in the region defined by π₯ β β and π¦ > 0, this shows that the IVP has no
unique solution but it has infinite solutions.
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(1.2) Initial-Value Problems
EXAMPLE 3
According to the Existence and Uniqueness Theorem, determine whether the IVP
has a unique solution.
SOLUTION:
ππ¦
= π₯π¦1/2 ,
ππ₯
1
π¦ (2) = 1
1 β π(π₯, π¦) = π₯π¦ 2 = π₯ βπ¦ is continuous on {(π₯, π¦): π₯ β β and π¦ β [0, β)}.
ππ
π₯
π₯
2β
= 1=
is continuous on {(π₯, π¦): π₯ β β and π¦ β (0, β)}.
ππ¦
2
π¦
β
2π¦ 2
Since (2,1) is in the region defined by π₯ β β and π¦ > 0, this shows that the IVP has a unique
solution.
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(1.2) Initial-Value Problems
Exercises 1.2: Page 17
(ππ) Determine a region of the π₯π¦-plane for which the given differential equation would have a
unique solution whose graph passes through a point (π₯0 , π¦0 ) in the region.
SOLUTION:
ππ¦
= βπ₯π¦
ππ₯
1 β π(π₯, π¦) = βπ₯π¦ is continuous on either {(π₯, π¦): π₯ β [0, β) and π¦ β [0, β)} or
{(π₯, π¦): π₯ β (ββ, 0] and π¦ β (ββ, 0]}.
2β
ππ 1 π₯
= β
ππ¦ 2 π¦
is continuous on either {(π₯, π¦): π₯ β [0, β) and π¦ β (0, β)} or
{(π₯, π¦): π₯ β (ββ, 0] and π¦ β (ββ, 0)}.
Thus, the differential equation will have a unique solution in any region where π₯ > 0 and π¦ > 0
or where π₯ < 0 and π¦ < 0.
------------------------------------------------------------------------------------------------------------------(ππ) Determine whether Theorem 1.2.1 guarantees that the differential equation
π¦ β² = βπ¦ 2 β 9
possesses a unique solution through the given point (2, β3).
SOLUTION:
1 β π(π₯, π¦) = βπ¦ 2 β 9 is continuous on {(π₯, π¦): π₯ β β and π¦ β (ββ, β3] βͺ [3, β)}.
ππ
2π¦
π¦
2β
=
=
is continuous on {(π₯, π¦): π₯ β β and π¦ β (ββ, β3) βͺ (3, β)}.
ππ¦ 2βπ¦ 2 β 9 βπ¦ 2 β 9
Since (2, β3) is not in either of the regions defined by π¦ < β3 or π¦ > 3, so there is no
guarantee of a unique solution through (2, β3).
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(1.2) Initial-Value Problems
Exercises 1.2: Page 17 (Homework)
(π) In the following problem, π¦ = 1/(π₯ 2 + π) is a one-parameter family of solutions of the first-
order DE π¦ β² + 2π₯π¦ 2 = 0. Find a solution of the first-order IVP consisting of this differential
equation and the given initial condition. Give the largest interval πΌ over which the solution is
defined.
1
π¦ ( ) = β4
2
------------------------------------------------------------------------------------------------------------------(π) In the following problem, π₯ = π1 cos π‘ + π2 sin π‘ is a two-parameter family of solutions of the
second-order DE π₯ β²β² + π₯ = 0. Find a solution of the second-order IVP consisting of this
differential equation and the given initial conditions.
π
1
π
π₯ ( ) = , π₯β² ( ) = 0
6
2
6
------------------------------------------------------------------------------------------------------------------In the following problems, determine a region of the π₯π¦-plane for which the given differential
equation would have a unique solution whose graph passes through a point (π₯0 , π¦0 ) in the region.
ππ¦
= π¦ 2/3
ππ₯
(ππ) (1 + π¦ 3 )π¦ β² = π₯ 2
------------------------------------------------------------------------------------------------------------------(ππ)
(ππ) In the following problem, determine whether Theorem 1.2.1 guarantees that the differential
equation
π¦ β² = βπ¦ 2 β 9
possesses a unique solution through the given point (1, 4).
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