| Topic I | Introduction & Summary for the Section |
| Topic II | Recalling the { linear mapping } relation |
| Topic III | Linear Mapping Basics |
| Topic IV | Setting up the { Unit-Sphere } in { Reference Frame B } |
| Topic V | Setting up the quantity { Rho-T } |
| Topic VI | Identifying the Maximum |
| Topic VII | An Analysis of the Maximum |
| Topic VIII | The 'mapped' Ellipsoid |
In this section, we shall take a further look at the { linear mapping } relation we have previously developed in { Section 1 } .
Our key finding here is that :
Let us now recall the { linear mapping } relation we have previously developed in { Section 1 } :




Let us now set up two (2) { 3-Dimensional reference frames } :
,
,
} ,
as per these two (2) diagrams below :
& 
& 
Let us now focus on the following three (3) relations of particular interests :




This then maps the { unit-vector } [
] in { Reference Frame B } onto the [
] vector in { Reference Frame A } , with :




This then maps the { unit-vector } [
] in { Reference Frame B } onto the [
] vector in { Reference Frame A } , with :




This then maps the { unit-vector } [
] in { Reference Frame B } onto the [
] vector in { Reference Frame A } , with :
as per this pair of diagrams below :
& 
Let us now set up a { unit-sphere } in { Reference Frame B } so that :
} is a point on this { unit-sphere } surface , as per these two (2) diagrams below :
& 
The { unit-vector }
is then given by :

,
,
} satisfying the governing equation for the { unit-sphere } , i.e. :

The { unit-vector } {
} in { Reference Frame B } is then mapped onto the vector {
} in { Reference Frame A } , as per this pair of diagrams below :
& 
We shall now identify / re-label the vector {
} as the vector {
} , and we can write :

And the mapping relation here is then :




yielding the relations :
Let us now introduce the scalar quantity {
} , such that :

] is then the size of the vector [
] .
We can then write :

yielding, on expansion :

Then, for all points on the { unit-sphere } in { Reference Frame B } , satisfying the condition :
there is a particular set of values for {
,
,
} such that the value of
is at a maximum.
Let us suppose that we were able to identify such a set of values for {
,
,
} such that the value of
is at a maximum.
We shall then label this set of values as the set {
,
,
} .
We then identify, in the diagrams below, points and vectors associated with this set , the set {
,
,
} , which in turn is associated with the highest value of
:
& 
in { Reference Frame B } , as identified by the points {
} & {
} respectively , is then given by :

in { Reference Frame B } then maps onto the vector
in { Reference Frame A } , as identified by the points {
} & {
} respectively . And
is given by :

where :



The scalar quantity / value
, i.e. :

is then the value of
associated with the set {
,
,
} and it is the highest value for
.
Let us now identify a { unit-circle } on the plane orthogonal to the { unit-vector }
, in { Reference Frame B } , as per the right-hand-side diagram below :
& 
This { unit-circle } in { Reference Frame B } then maps onto an { ellipse } in { Reference Frame A } , as per the left-hand-side diagram above.
Let the point, {
} , be a point on the { unit-circle } in { Reference Frame B } , as per right-hand-side diagram below :
& 
so that the vector
in { Reference Frame B } maps onto the vector
in { Reference Frame A } , as per the left-hand-side diagram above.
We then summarize the current situation as follows :
in { Reference Frame B } maps onto
in { Reference Frame A } ,
in { Reference Frame B } maps onto
in { Reference Frame A } ,
and the { unit-vectors }
&
in { Reference Frame B } are orthogonal to one-another.
This then is a situation of a { 2-Dimensional Planar Mapping } of :
as per this pair of diagrams below :
& 
( both the { 'new' unit-circle } & the { 'new' ellipse } are then marked in 'yellow-color' ) .
( The reader may wish to branch to Appendix B for a briefing on { 2-Dimensional Planar Mapping } at this point . )
We then identify the angle
as the angle
, as per the above left-hand-side diagram above.
Let us now investigate the three (3) possibilities for the value of
, as follows :
is less than { 90 degrees } :

In this case, the { unit-circle } maps onto an { ellipse } but {
} is not the maximum point .
is exactly { 90 degrees } :

In this case, the { unit-circle } maps onto an { ellipse } and {
} is indeed the maximum point .
is more than { 90 degrees } :

In this case, the { unit-circle } maps onto an { ellipse } but {
} is not the maximum point .
Thus, the { 2nd Possibility } is the only viable case if {
} is indeed the maximum point where
attains its highest value.
That is to say :
is always 90 degrees.
The original { unit-circle } ,
, in { Reference Frame B } ,
then maps onto an { ellipse } ,
, in { Reference Frame A } ;
as per this pair of diagrams below :
& 
We can then identify, via the procedure outlined in Appendix B on { 2-Dimensional Planar Mapping } :
&
, respectively ,
in { Reference Frame A } ,
and also :
&
in { Reference Frame B } that maps into these { major-axis } & { minor-axis } vectors in { Reference Frame A } , respectively,
as marked in the pair of diagrams immediately above.
We then have three (3) orthogonal { unit-vectors } in { Reference Frame B } mapping onto three (3) orthogonal vectors in { Reference Frame A } , i.e. :
,
, &
mapping onto :
,
, &
, respectively.
We can then construct the corresponding { unit-sphere } mapping onto the { ellipsoid } accordingly :
& 
We then also present this pair of diagrams :
& 
identifying the { axis of the ellipsoid } and the { corresponding axis of the unit-sphere } .
We note here that the orientation of the { 3-axis } for the { ellipsoid } and for the { corresponding unit-sphere } maynot , and may, be different.
In the next section, we shall briefly go thru the mechanics for the rotation of a set of { orthogonal unit-vector Basis } in a { 3-Dimensional Vector-Space } , before further investigating the { rotational effects } of the { ellipsoid } in { Section 4 } .