Basic Implementation details
Contents
Basic Implementation details¶
Coordinate Systems and Vectors¶
Currently, sympy.vector
is able to deal with the Cartesian (also called
rectangular), spherical and other curvilinear coordinate systems.
A 3D Cartesian coordinate system can be initialized in sympy.vector
as
>>> from sympy.vector import CoordSys3D
>>> N = CoordSys3D('N')
The string parameter to the constructor denotes the name assigned to the system, and will primarily be used for printing purposes.
Once a coordinate system (in essence, a CoordSys3D
instance)
has been defined, we can access the orthonormal unit vectors (i.e. the
\(\mathbf{\hat{i}}\), \(\mathbf{\hat{j}}\) and
\(\mathbf{\hat{k}}\) vectors) and coordinate variables/base
scalars (i.e. the \(\mathbf{x}\), \(\mathbf{y}\) and
\(\mathbf{z}\) variables) corresponding to it. We will talk
about coordinate variables in the later sections.
The basis vectors for the \(X\), \(Y\) and \(Z\)
axes can be accessed using the i
, j
and k
properties respectively.
>>> N.i
N.i
>>> type(N.i)
<class 'sympy.vector.vector.BaseVector'>
As seen above, the basis vectors are all instances of a class called
BaseVector
.
When a BaseVector
is multiplied by a scalar (essentially any
SymPy Expr
), we get a VectorMul
- the product of
a base vector and a scalar.
>>> 3*N.i
3*N.i
>>> type(3*N.i)
<class 'sympy.vector.vector.VectorMul'>
Addition of VectorMul
and BaseVectors
gives rise to
formation of VectorAdd
- except for special cases, ofcourse.
>>> v = 2*N.i + N.j
>>> type(v)
<class 'sympy.vector.vector.VectorAdd'>
>>> v - N.j
2*N.i
>>> type(v - N.j)
<class 'sympy.vector.vector.VectorMul'>
What about a zero vector? It can be accessed using the zero
attribute assigned to class Vector
. Since the notion of a zero
vector remains the same regardless of the coordinate system in
consideration, we use Vector.zero
wherever such a quantity is
required.
>>> from sympy.vector import Vector
>>> Vector.zero
0
>>> type(Vector.zero)
<class 'sympy.vector.vector.VectorZero'>
>>> N.i + Vector.zero
N.i
>>> Vector.zero == 2*Vector.zero
True
All the classes shown above - BaseVector
, VectorMul
,
VectorAdd
and VectorZero
are subclasses of Vector
.
You should never have to instantiate objects of any of the
subclasses of Vector
. Using the BaseVector
instances assigned to a
CoordSys3D
instance and (if needed) Vector.zero
as building blocks, any sort of vectorial expression can be constructed
with the basic mathematical operators +
, -
, *
.
and /
.
>>> v = N.i - 2*N.j
>>> v/3
1/3*N.i + (-2/3)*N.j
>>> v + N.k
N.i + (-2)*N.j + N.k
>>> Vector.zero/2
0
>>> (v/3)*4
4/3*N.i + (-8/3)*N.j
In addition to the elementary mathematical operations, the vector
operations of dot
and cross
can also be performed on
Vector
.
>>> v1 = 2*N.i + 3*N.j - N.k
>>> v2 = N.i - 4*N.j + N.k
>>> v1.dot(v2)
-11
>>> v1.cross(v2)
(-1)*N.i + (-3)*N.j + (-11)*N.k
>>> v2.cross(v1)
N.i + 3*N.j + 11*N.k
The &
and ^
operators have been overloaded for the
dot
and cross
methods respectively.
>>> v1 & v2
-11
>>> v1 ^ v2
(-1)*N.i + (-3)*N.j + (-11)*N.k
However, this is not the recommended way of performing these operations. Using the original methods makes the code clearer and easier to follow.
In addition to these operations, it is also possible to compute the
outer products of Vector
instances in sympy.vector
. More
on that in a little bit.
SymPy operations on Vectors¶
The SymPy operations of simplify
, trigsimp
, diff
,
and factor
work on Vector
objects, with the standard SymPy API.
In essence, the methods work on the measure numbers(The coefficients of the basis vectors) present in the provided vectorial expression.
>>> from sympy.abc import a, b, c
>>> from sympy import sin, cos, trigsimp, diff
>>> v = (a*b + a*c + b**2 + b*c)*N.i + N.j
>>> v.factor()
((a + b)*(b + c))*N.i + N.j
>>> v = (sin(a)**2 + cos(a)**2)*N.i - (2*cos(b)**2 - 1)*N.k
>>> trigsimp(v)
N.i + (-cos(2*b))*N.k
>>> v.simplify()
N.i + (-cos(2*b))*N.k
>>> diff(v, b)
(4*sin(b)*cos(b))*N.k
>>> from sympy import Derivative
>>> Derivative(v, b).doit()
(4*sin(b)*cos(b))*N.k
Integral
also works with Vector
instances, similar to
Derivative
.
>>> from sympy import Integral
>>> v1 = a*N.i + sin(a)*N.j - N.k
>>> Integral(v1, a)
(Integral(a, a))*N.i + (Integral(sin(a), a))*N.j + (Integral(-1, a))*N.k
>>> Integral(v1, a).doit()
a**2/2*N.i + (-cos(a))*N.j + (-a)*N.k
Points¶
As mentioned before, every coordinate system corresponds to a unique origin
point. Points, in general, have been implemented in sympy.vector
in the
form of the Point
class.
To access the origin of system, use the origin
property of the
CoordSys3D
class.
>>> from sympy.vector import CoordSys3D
>>> N = CoordSys3D('N')
>>> N.origin
N.origin
>>> type(N.origin)
<class 'sympy.vector.point.Point'>
You can instantiate new points in space using the locate_new
method of Point
. The arguments include the name(string) of the
new Point
, and its position vector with respect to the
‘parent’ Point
.
>>> from sympy.abc import a, b, c
>>> P = N.origin.locate_new('P', a*N.i + b*N.j + c*N.k)
>>> Q = P.locate_new('Q', -b*N.j)
Like Vector
, a user never has to expressly instantiate an object of
Point
. This is because any location in space (albeit relative) can be
pointed at by using the origin
of a CoordSys3D
as the
reference, and then using locate_new
on it and subsequent
Point
instances.
The position vector of a Point
with respect to another Point
can
be computed using the position_wrt
method.
>>> P.position_wrt(Q)
b*N.j
>>> Q.position_wrt(N.origin)
a*N.i + c*N.k
Additionally, it is possible to obtain the \(X\), \(Y\) and \(Z\)
coordinates of a Point
with respect to a CoordSys3D
in the form of a tuple. This is done using the express_coordinates
method.
>>> Q.express_coordinates(N)
(a, 0, c)
Dyadics¶
A dyadic, or dyadic tensor, is a second-order tensor formed by the
juxtaposition of pairs of vectors. Therefore, the outer products of vectors
give rise to the formation of dyadics. Dyadic tensors have been implemented
in sympy.vector
in the Dyadic
class.
Once again, you never have to instantiate objects of Dyadic
.
The outer products of vectors can be computed using the outer
method of Vector
. The |
operator has been overloaded for
outer
.
>>> from sympy.vector import CoordSys3D
>>> N = CoordSys3D('N')
>>> N.i.outer(N.j)
(N.i|N.j)
>>> N.i|N.j
(N.i|N.j)
Similar to Vector
, Dyadic
also has subsequent subclasses like
BaseDyadic
, DyadicMul
, DyadicAdd
. As with Vector
,
a zero dyadic can be accessed from Dyadic.zero
.
All basic mathematical operations work with Dyadic
too.
>>> dyad = N.i.outer(N.k)
>>> dyad*3
3*(N.i|N.k)
>>> dyad - dyad
0
>>> dyad + 2*(N.j|N.i)
(N.i|N.k) + 2*(N.j|N.i)
dot
and cross
also work among Dyadic
instances as well as
between a Dyadic
and Vector
(and also vice versa) - as per the
respective mathematical definitions. As with Vector
, &
and
^
have been overloaded for dot
and cross
.
>>> d = N.i.outer(N.j)
>>> d.dot(N.j|N.j)
(N.i|N.j)
>>> d.dot(N.i)
0
>>> d.dot(N.j)
N.i
>>> N.i.dot(d)
N.j
>>> N.k ^ d
(N.j|N.j)