7. Forms of representation of a line in the space.
There
are different ways of representation of a line in the space in some
Cartesian system of coordinates
.
1.
An
equation of a line in parametric form.
Let a point with the radius-vector
lies on a line in the space having non-zero directing vector
and passing through a point
.
Then collinearity of vectors
and
implies that an equation of line in the space must have the form:
.
2.
An
equation of a line in canonic form.
If we exclude parameter
from the scalar record of the equation
:
then we obtain so-calledcanonic
equation
of line:
.
3.
An
equation of a line passing through two non-coinciding points
and
.
Since
directing vector of the line
is collinear to vector
,
an equation of line in vector form can be represented as
or
.
Excluding
parameter
,
we obtain an equation in the coordinate form:
only
if
.
4.
An
equation of a line in the first vector form.
A line in the space can be given as a line of intersection of two
planes
and
where
and
are non-collinear, normal vectors of these planes, and
and
are some numbers.
If
it is known a point
which is passed through by a given line then the radius-vector of any
point of this line satisfies to the following system of equations:
or in the coordinate form:
.
5.
An
equation of a line in the second vector form.
A line in the space can be given by means of the condition of
collinearity of vectors
and
,
i.e.
or
where
.
In
an orthonormal system of coordinates
this equation of line in the space is:
or
.
At
last, the distance
between some point with the radius-vector
and a line
in the space can be found by using that
is the area of parallelogram constructed on the pair of vectors is
equal to the module of their vector product.

.
8. Curves of the second order in plane: theorem on canonic forms (case B = 0). Canonic system.
Let
an orthonormal system of coordinates
and some curve
be given on a plane.
A
curve
is called analgebraic
curve of the second order
if its equation in a given system of coordinates has the form:

where
numbers
and
are not equal to zero simultaneously (
),
and
and
are the coordinates of the radius-vector of a point lying in the
curve
.
Introduce
the following notation:
.
Theorem
1.
For every curve of the second order there exists an orthonormal
system of coordinates
in which an equation of this curve has (for
)
one of the following nine (calledcanonic)
forms:
|
Type of curve |
|
|
|
|
Empty sets |
|
|
|
|
Points |
|
|
|
|
Coinciding lines |
|
|
|
|
Non-coinciding lines |
|
|
|
|
Curves |
Ellipse
|
Hyperbola
|
Parabola
|
Remark
1.
Curves of the second order for which
are related to anelliptic
type,
curves with
– to ahyperbolic
type,
and curves with
– to aparabolic
type.
Remark 2. In order to find the canonic system of coordinates (i.e. the system of coordinates in which an equation has a canonic form) we write each of transition formulas, substitute them each other and obtain a final expression of the original coordinates through canonic ones:

The
coefficients of these formulas give the coordinates of the origin of
canonic system of coordinates
and its basis vectors
regarding to the original system.












