(1.2) Initial-Value Problems

(1.2) Initial-Value Problems
INTRODUCTION:
We are often interested in problems in which we seek a solution 𝑦(π‘₯) of a differential equation so that
𝑦(π‘₯) satisfies prescribed side conditionsβ€”that is, conditions imposed on the unknown 𝑦(π‘₯) or its
derivatives. On some interval 𝐼 containing π‘₯0 the problem
π‘†π‘œπ‘™π‘£π‘’:
𝑑𝑛 𝑦
= 𝑓(π‘₯, 𝑦, 𝑦 β€² , … , 𝑦 (π‘›βˆ’1) )
𝑑π‘₯ 𝑛
𝑆𝑒𝑏𝑗𝑒𝑐𝑑 π‘‘π‘œ:
𝑦(π‘₯0 ) = 𝑦0 , 𝑦 β€² (π‘₯0 ) = 𝑦1 , … , 𝑦 (π‘›βˆ’1) (π‘₯0 ) = π‘¦π‘›βˆ’1 ,
… … … … … … … … … … (1)
where 𝑦0 , 𝑦1 , … , π‘¦π‘›βˆ’1 are arbitrarily specified real constants, is called an initial-value problem
(IVP). The values of 𝑦(π‘₯) and its first 𝑛 βˆ’ 1 derivatives at a single point π‘₯0 , 𝑦(π‘₯0 ) = 𝑦0 , 𝑦 β€² (π‘₯0 ) =
𝑦1 , … , 𝑦 (π‘›βˆ’1) (π‘₯0 ) = π‘¦π‘›βˆ’1 , are called initial conditions.
FIRST- AND SECOND-ORDER IVPS:
The problem given in (1) is also called an 𝒏th-order initial-value problem. For example,
π‘†π‘œπ‘™π‘£π‘’:
𝑆𝑒𝑏𝑗𝑒𝑐𝑑 π‘‘π‘œ:
and
π‘†π‘œπ‘™π‘£π‘’:
𝑆𝑒𝑏𝑗𝑒𝑐𝑑 π‘‘π‘œ:
𝑑𝑦
= 𝑓 (π‘₯, 𝑦)
𝑑π‘₯
… … … … … … … … … … (2)
𝑦(π‘₯0 ) = 𝑦0
𝑑2 𝑦
= 𝑓 (π‘₯, 𝑦, 𝑦 β€² )
2
𝑑π‘₯
𝑦(π‘₯0 ) = 𝑦0 , 𝑦 β€² (π‘₯0 ) = 𝑦1
… … … … … … … … … … (3)
are first- and second-order initial-value problems, respectively.
THEOREM 1.2.1 (Existence of a Unique Solution)
Let 𝑅 be a rectangular region in the π‘₯𝑦-plane defined by π‘Ž ≀ π‘₯ ≀ 𝑏, 𝑐 ≀ 𝑦 ≀ 𝑑 that contains the
point (π‘₯0 , 𝑦0 ) in its interior. If 𝑓 (π‘₯, 𝑦) and πœ•π‘“ β„πœ•π‘¦ are continuous on 𝑅 , then there exists some interval
𝐼0 : (π‘₯0 βˆ’ β„Ž, π‘₯0 + β„Ž), β„Ž > 0, contained in [π‘Ž, 𝑏], and a unique function 𝑦(π‘₯), defined on 𝐼0 , that is a
solution of the initial-value problem (2).
𝑑𝑦
Roughly speaking, if we have the IVP
= 𝑓 (π‘₯, 𝑦), 𝑦(π‘₯0 ) = 𝑦0 , then we have 3 cases explain the
𝑑π‘₯
theorem which are follows:
ο‚· If 𝑓 (π‘₯, 𝑦) and πœ•π‘“/πœ•π‘¦ are continuous on a common domain 𝐼
β‡’ the solution of the IVP exists and unique.
ο‚· If 𝑓 (π‘₯, 𝑦) is only continuous on a domain 𝐼
β‡’ the solution of the IVP exists only. This means that the IVP has infinite solutions
ο‚· If 𝑓 (π‘₯, 𝑦) is discontinuous on a domain 𝐼
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‘₯ = 𝑐1 cos 4𝑑 + 𝑐2 sin 4𝑑
is a two-parameter family of solutions of
π‘₯ β€²β€² + 16π‘₯ = 0.
Find a solution of the initial-value problem
πœ‹
πœ‹
π‘₯ β€²β€² + 16π‘₯ = 0, π‘₯ ( ) = βˆ’2, π‘₯ β€² ( ) = 1.
2
2
… … … … … … … … … … (4)
SOLUTION:
We first find π‘₯ β€² and π‘₯ β€²β€² using the general solution π‘₯ = 𝑐1 cos 4𝑑 + 𝑐2 sin 4𝑑 , we obtain
π‘₯ β€² = βˆ’4𝑐1 sin 4𝑑 + 4𝑐2 cos 4𝑑
and
πœ‹
π‘₯ β€²β€² = βˆ’16𝑐1 cos 4𝑑 βˆ’ 16𝑐2 sin 4𝑑.
Then, we apply π‘₯ ( ) = βˆ’2 to the given family of solutions:
2
πœ‹
πœ‹
πœ‹
π‘₯ ( ) = 𝑐1 cos (4 ( )) + 𝑐2 sin (4 ( )) = 𝑐1 cos 2πœ‹ + 𝑐2 sin 2πœ‹ = 𝑐1 (1) + 𝑐2 (0) = 𝑐1 = βˆ’2.
2
2
2
πœ‹
Hence, 𝑐1 = βˆ’2. Similarly, we next apply π‘₯ β€² ( ) = 1 to the two-parameter family
2
π‘₯ β€² = βˆ’4𝑐1 sin 4𝑑 + 4𝑐2 cos 4𝑑.
So,
πœ‹
πœ‹
πœ‹
π‘₯ β€² ( ) = βˆ’4(βˆ’2) sin (4 ( )) + 4𝑐2 cos (4 ( )) = 8 sin 2πœ‹ + 4𝑐2 cos 2πœ‹ = 8(0) + 4𝑐2 (1) = 4𝑐2 = 1.
2
2
2
1
Thus, 𝑐2 = . Hence,
4
1
π‘₯ = βˆ’2 cos 4𝑑 + sin 4𝑑
4
is a solution of (4).
EXAMPLE 2
According to the Existence and Uniqueness Theorem, determine whether the IVP
has a unique solution.
SOLUTION:
𝑑𝑦
= π‘₯𝑦1/2 ,
𝑑π‘₯
𝑦 (0) = 0
1
1 βˆ’ 𝑓(π‘₯, 𝑦) = π‘₯𝑦 2 = π‘₯ βˆšπ‘¦ is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ [0, ∞)}.
πœ•π‘“
π‘₯
π‘₯
2βˆ’
= 1=
is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ (0, ∞)}.
πœ•π‘¦ 2𝑦 2 2βˆšπ‘¦
Since (0,0) is not in the region defined by π‘₯ ∈ ℝ and 𝑦 > 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:
𝑑𝑦
= π‘₯𝑦1/2 ,
𝑑π‘₯
1
𝑦 (2) = 1
1 βˆ’ 𝑓(π‘₯, 𝑦) = π‘₯𝑦 2 = π‘₯ βˆšπ‘¦ is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ [0, ∞)}.
πœ•π‘“
π‘₯
π‘₯
2βˆ’
= 1=
is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ (0, ∞)}.
πœ•π‘¦
2
𝑦
√
2𝑦 2
Since (2,1) is in the region defined by π‘₯ ∈ ℝ and 𝑦 > 0, this shows that the IVP has a unique
solution.
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(1.2) Initial-Value Problems
Exercises 1.2: Page 17
(πŸπŸ–) Determine a region of the π‘₯𝑦-plane for which the given differential equation would have a
unique solution whose graph passes through a point (π‘₯0 , 𝑦0 ) in the region.
SOLUTION:
𝑑𝑦
= √π‘₯𝑦
𝑑π‘₯
1 βˆ’ 𝑓(π‘₯, 𝑦) = √π‘₯𝑦 is continuous on either {(π‘₯, 𝑦): π‘₯ ∈ [0, ∞) and 𝑦 ∈ [0, ∞)} or
{(π‘₯, 𝑦): π‘₯ ∈ (βˆ’βˆž, 0] and 𝑦 ∈ (βˆ’βˆž, 0]}.
2βˆ’
πœ•π‘“ 1 π‘₯
= √
πœ•π‘¦ 2 𝑦
is continuous on either {(π‘₯, 𝑦): π‘₯ ∈ [0, ∞) and 𝑦 ∈ (0, ∞)} or
{(π‘₯, 𝑦): π‘₯ ∈ (βˆ’βˆž, 0] and 𝑦 ∈ (βˆ’βˆž, 0)}.
Thus, the differential equation will have a unique solution in any region where π‘₯ > 0 and 𝑦 > 0
or where π‘₯ < 0 and 𝑦 < 0.
------------------------------------------------------------------------------------------------------------------(πŸπŸ•) Determine whether Theorem 1.2.1 guarantees that the differential equation
𝑦 β€² = βˆšπ‘¦ 2 βˆ’ 9
possesses a unique solution through the given point (2, βˆ’3).
SOLUTION:
1 βˆ’ 𝑓(π‘₯, 𝑦) = βˆšπ‘¦ 2 βˆ’ 9 is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ (βˆ’βˆž, βˆ’3] βˆͺ [3, ∞)}.
πœ•π‘“
2𝑦
𝑦
2βˆ’
=
=
is continuous on {(π‘₯, 𝑦): π‘₯ ∈ ℝ and 𝑦 ∈ (βˆ’βˆž, βˆ’3) βˆͺ (3, ∞)}.
πœ•π‘¦ 2βˆšπ‘¦ 2 βˆ’ 9 βˆšπ‘¦ 2 βˆ’ 9
Since (2, βˆ’3) is not in either of the regions defined by 𝑦 < βˆ’3 or 𝑦 > 3, so there is no
guarantee of a unique solution through (2, βˆ’3).
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(1.2) Initial-Value Problems
Exercises 1.2: Page 17 (Homework)
(πŸ”) In the following problem, 𝑦 = 1/(π‘₯ 2 + 𝑐) is a one-parameter family of solutions of the first-
order DE 𝑦 β€² + 2π‘₯𝑦 2 = 0. Find a solution of the first-order IVP consisting of this differential
equation and the given initial condition. Give the largest interval 𝐼 over which the solution is
defined.
1
𝑦 ( ) = βˆ’4
2
------------------------------------------------------------------------------------------------------------------(πŸ—) In the following problem, π‘₯ = 𝑐1 cos 𝑑 + 𝑐2 sin 𝑑 is a two-parameter family of solutions of the
second-order DE π‘₯ β€²β€² + π‘₯ = 0. Find a solution of the second-order IVP consisting of this
differential equation and the given initial conditions.
πœ‹
1
πœ‹
π‘₯ ( ) = , π‘₯β€² ( ) = 0
6
2
6
------------------------------------------------------------------------------------------------------------------In the following problems, determine a region of the π‘₯𝑦-plane for which the given differential
equation would have a unique solution whose graph passes through a point (π‘₯0 , 𝑦0 ) in the region.
𝑑𝑦
= 𝑦 2/3
𝑑π‘₯
(𝟐𝟐) (1 + 𝑦 3 )𝑦 β€² = π‘₯ 2
------------------------------------------------------------------------------------------------------------------(πŸπŸ•)
(πŸπŸ“) In the following problem, determine whether Theorem 1.2.1 guarantees that the differential
equation
𝑦 β€² = βˆšπ‘¦ 2 βˆ’ 9
possesses a unique solution through the given point (1, 4).
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