5. INTRODUCTION:
Let π’ = π’(π₯1, . . , π₯π) be a function of n-independent variable π₯1, β¦ , π₯π.
A partial differential equation that contain the independent variable
π₯1, β¦ , π₯π , the dependent variable or the unknown function u and its
partial derivatives up to some order . It has the form
πΉ π₯1, β¦ , π₯π, π’, π’π₯1
, . . , π’π₯π
, π’π₯1π₯1
, β¦ . , π’π₯ππ₯π
, β¦ = 0
Where F is given function and π’π₯π
=
ππ’
ππ₯π
, π’π₯ππ₯π
=
π2π’
ππ₯πππ₯π
π, π = 1, β¦ , π
are the partial derivatives of u. The order of partial differential equation
is the order of the highest derivatives which is appear in the equation.
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6. Almost Linear Second Order
Equation In n-Independent Variables:
An almost-linear second order equation in n-independent variables π₯1, π₯2, β¦ . . π₯π is
of the form
π=1
π
π=1
π
π΄ππ
π2π’
ππ₯πππ₯π
+ M π₯1, π₯2, β¦ . π₯π, π’, π’π₯1
, π’π₯2
, β¦ , π’π₯π
= 0 (1)
It is assumed that the coefficient π΄ππ are real-valued continuously differentiable
function of π₯1, π₯2, β¦ . , π₯π and that π΄ππ = π΄ππ, i,j=1,2,β¦,n.
The linear operator
πΏ = π=1
π
π=1
π
π΄πππ·π₯π
π·π₯π
where π·π₯π
=
π
ππ₯π
π = 1,2, β¦ . , π
π·π₯π
=
π
ππ₯π
π = 1,2, β¦ . , π
is called the principal part of the operator L appearing in equation (1).
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7. Classification based on the
characteristic form:
Classification based on the characteristic form
π π = π=1
π
π=1
π
π΄ππππππ (2)
It is understood that the function π΄ππ are evaluated at π₯1 = π₯10, β¦ β¦ . , π₯π = π₯π0 and
(π1, β¦ . , ππ) is a real n-tuple.
A well known property of such a real quadratic is that there exist a linear
transformation ππ = π=1
π
πππππ i=1,2,β¦,n where π = πππ is a non-singular matrix such
that π(π) is reduce to canonical form.
π π = π1
2
+ β― + ππ
2
β ππ+1
2
β β― β ππ+π
2
(3)
Where ππ β 0, π = 1,2, β¦ , π + π
π β₯ 0 is called the positive index in (3).
π β€ 0 is called the negative index.
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8. Continueβ¦..
Therefore the classification of the canonical form of the characteristic form of
equation (2).
Let
π = π΄π
be the non-singular linear transformation reducing the equation (2) to the
canonical form. Then the transformation
π¦ = π΄π
π₯
reducing equation (3) β
π=1
π
π£π¦ππ¦π
β π=1
π
π£π¦π+ππ¦π+π + πΉ π¦, π£, π»π£ = 0,
Where
π£ π¦ = π’( π΄π β1π¦).
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9. Continueβ¦..
And the number π = π + π is called rank of characteristic form Q at a point
π₯1 = π₯10, β¦ π₯π = π₯π0. The rank π β€ π , and r is called the rank of matrix π΄ = π΄ππ at the
point. The number v = π β π is called the nullity of the characteristic form, and π β₯ 0.
Thus π>0 if and only if the rank of matrix A is less then n that is if and only if A is a
singular matrix.
The important thing is that these numbers are invariant with respect to real
nonsingular linear transformations of the variable π1, π2 , β¦ , ππ that is they have the
same value regardless the mode of the reduction of the π π to the form in eqn (3).
At π₯1 = π₯10, β¦ , π₯π = π₯π0 the operator L (in equ 1) is said to be
1. Elliptic if π = 0, πππ πππ‘βππ π = 0 ππ π = 0
2. Hyperbolic if π = 0 πππ πππ‘βππ π = π β 1 πππ π = 1 ππ π = 1 πππ π = π β 1
3. Ultra hyperbolic if π = 0 πππ 1 < π < π β 1 (π π 1 < π < π β 1 )
4. Parabolic if π > 0
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10. Continueβ¦
β’ The operator L is elliptic at the point if and only if ,the characteristic form is definite ,
being either positive definite or negative definite .
β’ The form is positive definite if π(π) β₯ 0 holds for all real n-tuples ( π1, . . , ππ )
and π π = 0 if and only if π1 = β― = ππ = 0.
β’ The form is the negative definite if
π(π) β€ 0 .
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11. Explanation.
Question:
π π = π=1
π
π=1
π
π΄ππππππ (2)
We discuss this general form for n=2 and for n > 2.
Solution:
Case:1
For n=2
π π = π΄11π1
2
+ 2π΄12π1π2 + π΄22π2
2
This form is definite if and only if Ξ = π΄12
2
β π΄11π΄22 < 0.
Thus the criterion for ellipticity of L in the general case reduce in the particular case
n=2 to the criterion stated previously for the operator.
In the same way it follows that the criteria for the hyperbolicity and parabolicity
state above reduce to Ξ > 0 and Ξ = 0 respectively.
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12. continueβ¦.
β’ Case :2
If n>2, it is not possible in general to reduce Equ (1) to normal form in a
region. However in the special case where the coefficient π΄ππ are constant it is possible
to reduce the differential equation to normal form. Then equation (1) becomes
1. If L is Elliptic
Ξπ£ + ππ£ = πΉ(π₯1, β¦ , π₯π)
where βcβ is constant and Ξπ£ =
π2π£
ππ₯1
2 + β― +
π2π£
ππ₯π
2
2. If L is hyperbolic
π2π£
ππ₯1
2 + β― +
π2π£
ππ₯πβ1
2 β
π2π£
ππ₯π
2 + ππ£ = πΉ(π₯1, β¦ , π₯π)
3. If L is ultra hyperbolic the equation ca be reduce to normal form
π2π£
ππ₯1
2 + β― +
π2π£
ππ₯π
2 β
π2π£
ππ₯π+1
2 β β― β
π2π£
ππ₯π+π
2 + ππ£ = πΉ(π₯1, β¦ , π₯π)
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13. continueβ¦.
Where 1 < π < π β 1 πππ π + π = π .
4. If L is parabolic
π2π£
ππ₯1
2 + β― +
π2π£
ππ₯π
2 + π΅π+1
ππ£
ππ₯π+1
2 + β― + π΅π
ππ£
ππ₯π
+ ππ£ = πΉ(π₯1, . . . , π₯π)
where 0 < π < π.
If n=2 the normal written above in the hyperbolic case is
π2π£
ππ₯2 β
π2π£
ππ¦2 + ππ£ = πΉ π₯, π¦ .
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