=======================
Vector & ReferenceFrame
=======================


In :mod:`sympy.physics.vector`, vectors and reference frames are the "building blocks" of
dynamic systems. This document will describe these mathematically and describe
how to use them with this module's code.

Vector
======

A vector is a geometric object that has a magnitude (or length) and a
direction. Vectors in 3-space are often represented on paper as:

.. image:: vec_rep.*
   :height: 175
   :width: 350
   :align: center

Vector Algebra
==============

Vector algebra is the first topic to be discussed.

Two vectors are said to be equal if and only if (iff) they have the same
magnitude and orientation.

Vector Operations
-----------------
Multiple algebraic operations can be done with vectors: addition between
vectors, scalar multiplication, and vector multiplication.

Vector addition as based on the parallelogram law.

.. image:: vec_add.*
   :height: 200
   :width: 200
   :align: center

Vector addition is also commutative:

.. math::
  \mathbf{a} + \mathbf{b} &= \mathbf{b} + \mathbf{a} \\
  (\mathbf{a} + \mathbf{b}) + \mathbf{c} &= \mathbf{a} + (\mathbf{b} +
  \mathbf{c})

Scalar multiplication is the product of a vector and a scalar; the result is a
vector with the same orientation but whose magnitude is scaled by the scalar.
Note that multiplication by -1 is equivalent to rotating the vector by 180
degrees about an arbitrary axis in the plane perpendicular to the vector.

.. image:: vec_mul.*
   :height: 150
   :width: 200
   :align: center

A unit vector is simply a vector whose magnitude is equal to 1.  Given any
vector :math:`\mathbf{v}` we can define a unit vector as:

.. math::
  \mathbf{\hat{n}_v} = \frac{\mathbf{v}}{\Vert \mathbf{v} \Vert}

Note that every vector can be written as the product of a scalar and unit
vector.

Three vector products are implemented in :mod:`sympy.physics.vector`: the dot product, the
cross product, and the outer product.

The dot product operation maps two vectors to a scalar.  It is defined as:

.. math::
  \mathbf{a} \cdot \mathbf{b} = \Vert \mathbf{a} \Vert \Vert \mathbf{b}
  \Vert \cos(\theta)\\

where :math:`\theta` is the angle between :math:`\mathbf{a}` and
:math:`\mathbf{b}`.

The dot product of two unit vectors represent the magnitude of the common
direction; for other vectors, it is the product of the magnitude of the common
direction and the two vectors' magnitudes. The dot product of two perpendicular
is zero. The figure below shows some examples:

.. image:: vec_dot.*
   :height: 250
   :width: 450
   :align: center

The dot product is commutative:

.. math::
  \mathbf{a} \cdot \mathbf{b} = \mathbf{b} \cdot \mathbf{a}

The cross product vector multiplication operation of two vectors returns a
vector:

.. math::
  \mathbf{a} \times \mathbf{b} = \mathbf{c}

The vector :math:`\mathbf{c}` has the following properties: it's orientation is
perpendicular to both :math:`\mathbf{a}` and :math:`\mathbf{b}`, it's magnitude
is defined as :math:`\Vert \mathbf{c} \Vert = \Vert \mathbf{a} \Vert \Vert
\mathbf{b} \Vert \sin(\theta)` (where :math:`\theta` is the angle between
:math:`\mathbf{a}` and :math:`\mathbf{b}`), and has a sense defined by using
the right hand rule between :math:`\Vert \mathbf{a} \Vert \Vert \mathbf{b}
\Vert`. The figure below shows this:

.. image:: vec_cross.*
   :height: 350
   :width: 700
   :align: center

The cross product has the following properties:

It is not commutative:

.. math::
  \mathbf{a} \times \mathbf{b} &\neq \mathbf{b} \times \mathbf{a} \\
  \mathbf{a} \times \mathbf{b} &= - \mathbf{b} \times \mathbf{a}

and not associative:

.. math::
  (\mathbf{a} \times \mathbf{b} ) \times \mathbf{c} \neq \mathbf{a} \times
  (\mathbf{b} \times \mathbf{c})

Two parallel vectors will have a zero cross product.

The outer product between two vectors will not be not be discussed here, but
instead in the inertia section (that is where it is used). Other useful vector
properties and relationships are:

.. math::
  \alpha (\mathbf{a} + \mathbf{b}) &= \alpha \mathbf{a} + \alpha \mathbf{b}\\
  \mathbf{a} \cdot (\mathbf{b} + \mathbf{c}) &= \mathbf{a} \cdot \mathbf{b} +
  \mathbf{a} \cdot \mathbf{c}\\
  \mathbf{a} \times (\mathbf{b} + \mathbf{c}) &= \mathbf{a} \times \mathbf{b} +
  \mathbf{a} \times \mathbf{b}\\
  (\mathbf{a} \times \mathbf{b}) \cdot \mathbf{c} & \textrm{ gives the scalar
  triple product.}\\
  \mathbf{a} \times (\mathbf{b} \cdot \mathbf{c}) & \textrm{ does not work,
  as you cannot cross a vector and a scalar.}\\
  (\mathbf{a} \times \mathbf{b}) \cdot \mathbf{c} &= \mathbf{a} \cdot
  (\mathbf{b} \times \mathbf{c})\\
  (\mathbf{a} \times \mathbf{b}) \cdot \mathbf{c} &= (\mathbf{b} \times
  \mathbf{c}) \cdot \mathbf{a} = (\mathbf{c} \times \mathbf{a}) \cdot
  \mathbf{b}\\
  (\mathbf{a} \times \mathbf{b}) \times \mathbf{c} &= \mathbf{b}(\mathbf{a}
  \cdot \mathbf{c}) - \mathbf{a}(\mathbf{b} \cdot \mathbf{c})\\
  \mathbf{a} \times (\mathbf{b} \times \mathbf{c}) &= \mathbf{b}(\mathbf{a}
  \cdot \mathbf{c}) - \mathbf{c}(\mathbf{a} \cdot \mathbf{b})\\

Alternative Representation
--------------------------
If we have three non-coplanar unit vectors
:math:`\mathbf{\hat{n}_x},\mathbf{\hat{n}_y},\mathbf{\hat{n}_z}`,
we can represent any vector
:math:`\mathbf{a}` as :math:`\mathbf{a} = a_x \mathbf{\hat{n}_x} + a_y
\mathbf{\hat{n}_y} + a_z \mathbf{\hat{n}_z}`. In this situation
:math:`\mathbf{\hat{n}_x},\mathbf{\hat{n}_y},\mathbf{\hat{n}_z}`
are referred to as a basis.  :math:`a_x, a_y, a_z`
are called the measure numbers.
Usually the unit vectors are mutually perpendicular, in which case we can refer
to them as an orthonormal basis, and they are usually right-handed.

To test equality between two vectors, now we can do the following. With
vectors:

.. math::
  \mathbf{a} &= a_x \mathbf{\hat{n}_x} + a_y \mathbf{\hat{n}_y} + a_z
  \mathbf{\hat{n}_z}\\
  \mathbf{b} &= b_x \mathbf{\hat{n}_x} + b_y \mathbf{\hat{n}_y} + b_z
  \mathbf{\hat{n}_z}\\

We can claim equality if: :math:`a_x = b_x, a_y = b_y, a_z = b_z`.

Vector addition is then represented, for the same two vectors, as:

.. math::
  \mathbf{a} + \mathbf{b} = (a_x + b_x)\mathbf{\hat{n}_x} + (a_y + b_y)
  \mathbf{\hat{n}_y} + (a_z + b_z) \mathbf{\hat{n}_z}

Multiplication operations are now defined as:

.. math::
  \alpha \mathbf{b} &= \alpha b_x \mathbf{\hat{n}_x} + \alpha b_y
  \mathbf{\hat{n}_y} + \alpha b_z \mathbf{\hat{n}_z}\\
  \mathbf{a} \cdot \mathbf{b} &= a_x b_x + a_y b_y + a_z b_z\\
  \mathbf{a} \times \mathbf{b} &=
  \textrm{det }\begin{bmatrix} \mathbf{\hat{n}_x} & \mathbf{\hat{n}_y} &
  \mathbf{\hat{n}_z} \\ a_x & a_y & a_z \\ b_x & b_y & b_z \end{bmatrix}\\
  (\mathbf{a} \times \mathbf{b}) \cdot \mathbf{c} &=
  \textrm{det }\begin{bmatrix} a_x & a_y & a_z \\ b_x & b_y & b_z \\ c_x & c_y
  & c_z \end{bmatrix}\\

To write a vector in a given basis, we can do the follow:

.. math::
  \mathbf{a} = (\mathbf{a}\cdot\mathbf{\hat{n}_x})\mathbf{\hat{n}_x} +
  (\mathbf{a}\cdot\mathbf{\hat{n}_y})\mathbf{\hat{n}_y} +
  (\mathbf{a}\cdot\mathbf{\hat{n}_z})\mathbf{\hat{n}_z}\\


Examples
--------
Some numeric examples of these operations follow:

.. math::
  \mathbf{a} &= \mathbf{\hat{n}_x} + 5 \mathbf{\hat{n}_y}\\
  \mathbf{b} &= \mathbf{\hat{n}_y} + \alpha \mathbf{\hat{n}_z}\\
  \mathbf{a} + \mathbf{b} &= \mathbf{\hat{n}_x} + 6 \mathbf{\hat{n}_y} + \alpha
  \mathbf{\hat{n}_z}\\
  \mathbf{a} \cdot \mathbf{b} &= 5\\
  \mathbf{a} \cdot \mathbf{\hat{n}_y} &= 5\\
  \mathbf{a} \cdot \mathbf{\hat{n}_z} &= 0\\
  \mathbf{a} \times \mathbf{b} &= 5 \alpha \mathbf{\hat{n}_x} - \alpha
  \mathbf{\hat{n}_y} + \mathbf{\hat{n}_z}\\
  \mathbf{b} \times \mathbf{a} &= -5 \alpha \mathbf{\hat{n}_x} + \alpha
  \mathbf{\hat{n}_y} - \mathbf{\hat{n}_z}\\


Vector Calculus
===============
To deal with the calculus of vectors with moving object, we have to introduce
the concept of a reference frame. A classic example is a train moving along its
tracks, with you and a friend inside. If both you and your friend are sitting,
the relative velocity between the two of you is zero. From an observer outside
the train, you will both have velocity though.

We will now apply more rigor to this definition. A reference frame is a virtual
"platform" which we choose to observe vector quantities from. If we have a
reference frame :math:`\mathbf{N}`, vector :math:`\mathbf{a}` is said to be
fixed in the frame :math:`\mathbf{N}` if none of its properties ever change
when observed from :math:`\mathbf{N}`. We will typically assign a fixed
orthonormal basis vector set with each reference frame; :math:`\mathbf{N}` will
have :math:`\mathbf{\hat{n}_x}, \mathbf{\hat{n}_y},\mathbf{\hat{n}_z}` as its
basis vectors.

Derivatives of Vectors
----------------------

A vector which is not fixed in a reference frame therefore has changing
properties when observed from that frame. Calculus is the study of change, and
in order to deal with the peculiarities of vectors fixed and not fixed in
different reference frames, we need to be more explicit in our definitions.

.. image:: vec_fix_notfix.*
   :height: 300
   :width: 450
   :align: center

In the above figure, we have vectors :math:`\mathbf{c,d,e,f}`. If one were to
take the derivative of :math:`\mathbf{e}` with respect to :math:`\theta`:

.. math::
  \frac{d \mathbf{e}}{d \theta}

it is not clear what the derivative is. If you are observing from frame
:math:`\mathbf{A}`, it is clearly non-zero. If you are observing from frame
:math:`\mathbf{B}`, the derivative is zero. We will therefore introduce the
frame as part of the derivative notation:

.. math::
  \frac{^{\mathbf{A}} d \mathbf{e}}{d \theta} &\neq 0 \textrm{,
  the derivative of } \mathbf{e} \textrm{ with respect to } \theta
  \textrm{ in the reference frame } \mathbf{A}\\
  \frac{^{\mathbf{B}} d \mathbf{e}}{d \theta} &= 0 \textrm{,
   the derivative of } \mathbf{e} \textrm{ with respect to } \theta
  \textrm{ in the reference frame } \mathbf{B}\\
  \frac{^{\mathbf{A}} d \mathbf{c}}{d \theta} &= 0 \textrm{,
   the derivative of } \mathbf{c} \textrm{ with respect to } \theta
  \textrm{ in the reference frame } \mathbf{A}\\
  \frac{^{\mathbf{B}} d \mathbf{c}}{d \theta} &\neq 0 \textrm{,
   the derivative of } \mathbf{c} \textrm{ with respect to } \theta
  \textrm{ in the reference frame } \mathbf{B}\\

Here are some additional properties of derivatives of vectors in specific
frames:

.. math::
  \frac{^{\mathbf{A}} d}{dt}(\mathbf{a} + \mathbf{b}) &= \frac{^{\mathbf{A}}
  d\mathbf{a}}{dt} + \frac{^{\mathbf{A}} d\mathbf{b}}{dt}\\
  \frac{^{\mathbf{A}} d}{dt}\gamma \mathbf{a} &= \frac{ d \gamma}{dt}\mathbf{a}
  + \gamma\frac{^{\mathbf{A}} d\mathbf{a}}{dt}\\
  \frac{^{\mathbf{A}} d}{dt}(\mathbf{a} \times \mathbf{b}) &=
  \frac{^{\mathbf{A}} d\mathbf{a}}{dt} \times \mathbf{b} +
  \mathbf{a} \times \frac{^{\mathbf{A}} d\mathbf{b}}{dt}\\

Relating Sets of Basis Vectors
------------------------------

We need to now define the relationship between two different reference frames;
or how to relate the basis vectors of one frame to another. We can do this
using a direction cosine matrix (DCM). The direction cosine matrix relates
the basis vectors of one frame to another, in the following fashion:

.. math::
  \begin{bmatrix}
  \mathbf{\hat{a}_x} \\ \mathbf{\hat{a}_y} \\ \mathbf{\hat{a}_z} \\
  \end{bmatrix}  =
  \begin{bmatrix} ^{\mathbf{A}} \mathbf{C}^{\mathbf{B}} \end{bmatrix}
  \begin{bmatrix}
  \mathbf{\hat{b}_x} \\ \mathbf{\hat{b}_y} \\ \mathbf{\hat{b}_z} \\
  \end{bmatrix}

When two frames (say, :math:`\mathbf{A}` & :math:`\mathbf{B}`) are initially
aligned, then one frame has all of its basis vectors rotated around an axis
which is aligned with a basis vector, we say the frames are related by a simple
rotation. The figure below shows this:

.. image:: simp_rot.*
   :height: 250
   :width: 250
   :align: center

The above rotation is a simple rotation about the Z axis by an angle
:math:`\theta`. Note that after the rotation, the basis vectors
:math:`\mathbf{\hat{a}_z}` and :math:`\mathbf{\hat{b}_z}` are still aligned.

This rotation can be characterized by the following direction cosine matrix:

.. math::

  ^{\mathbf{A}}\mathbf{C}^{\mathbf{B}} =
  \begin{bmatrix}
  \cos(\theta) & - \sin(\theta) & 0\\
  \sin(\theta) & \cos(\theta) & 0\\
  0 & 0 & 1\\
  \end{bmatrix}

Simple rotations about the X and Y axes are defined by:

.. math::

  \textrm{DCM for x-axis rotation: }
  \begin{bmatrix}
  1 & 0 & 0\\
  0 & \cos(\theta) & -\sin(\theta)\\
  0 & \sin(\theta) & \cos(\theta)
  \end{bmatrix}

  \textrm{DCM for y-axis rotation: }
  \begin{bmatrix}
  \cos(\theta) & 0 & \sin(\theta)\\
  0 & 1 & 0\\
  -\sin(\theta) & 0 & \cos(\theta)\\
  \end{bmatrix}

Rotation in the positive direction here will be defined by using the right-hand
rule.

The direction cosine matrix is also involved with the definition of the dot
product between sets of basis vectors. If we have two reference frames with
associated basis vectors, their direction cosine matrix can be defined as:

.. math::

  \begin{bmatrix}
  C_{xx} & C_{xy} & C_{xz}\\
  C_{yx} & C_{yy} & C_{yz}\\
  C_{zx} & C_{zy} & C_{zz}\\
  \end{bmatrix} =
  \begin{bmatrix}
  \mathbf{\hat{a}_x}\cdot\mathbf{\hat{b}_x} &
  \mathbf{\hat{a}_x}\cdot\mathbf{\hat{b}_y} &
  \mathbf{\hat{a}_x}\cdot\mathbf{\hat{b}_z}\\
  \mathbf{\hat{a}_y}\cdot\mathbf{\hat{b}_x} &
  \mathbf{\hat{a}_y}\cdot\mathbf{\hat{b}_y} &
  \mathbf{\hat{a}_y}\cdot\mathbf{\hat{b}_z}\\
  \mathbf{\hat{a}_z}\cdot\mathbf{\hat{b}_x} &
  \mathbf{\hat{a}_z}\cdot\mathbf{\hat{b}_y} &
  \mathbf{\hat{a}_z}\cdot\mathbf{\hat{b}_z}\\
  \end{bmatrix}

Additionally, the direction cosine matrix is orthogonal, in that:

.. math::
  ^{\mathbf{A}}\mathbf{C}^{\mathbf{B}} =
  (^{\mathbf{B}}\mathbf{C}^{\mathbf{A}})^{-1}\\ =
  (^{\mathbf{B}}\mathbf{C}^{\mathbf{A}})^T\\

If we have reference frames :math:`\mathbf{A}` and :math:`\mathbf{B}`, which in
this example have undergone a simple z-axis rotation by an amount
:math:`\theta`, we will have two sets of basis vectors. We can then define two
vectors: :math:`\mathbf{a} = \mathbf{\hat{a}_x} + \mathbf{\hat{a}_y} +
\mathbf{\hat{a}_z}` and :math:`\mathbf{b} = \mathbf{\hat{b}_x} +
\mathbf{\hat{b}_y} + \mathbf{\hat{b}_z}`. If we wish to express
:math:`\mathbf{b}` in the :math:`\mathbf{A}` frame, we do the following:

.. math::
  \mathbf{b} &= \mathbf{\hat{b}_x} + \mathbf{\hat{b}_y} + \mathbf{\hat{b}_z}\\
  \mathbf{b} &= \begin{bmatrix}\mathbf{\hat{a}_x}\cdot (\mathbf{\hat{b}_x} +
  \mathbf{\hat{b}_y} + \mathbf{\hat{b}_z})\end{bmatrix} \mathbf{\hat{a}_x} +
  \begin{bmatrix}\mathbf{\hat{a}_y}\cdot (\mathbf{\hat{b}_x} + \mathbf{\hat{b}_y}
  + \mathbf{\hat{b}_z})\end{bmatrix} \mathbf{\hat{a}_y} +
  \begin{bmatrix}\mathbf{\hat{a}_z}\cdot (\mathbf{\hat{b}_x} + \mathbf{\hat{b}_y}
  + \mathbf{\hat{b}_z})\end{bmatrix} \mathbf{\hat{a}_z}\\ \mathbf{b} &=
  (\cos(\theta) - \sin(\theta))\mathbf{\hat{a}_x} +
  (\sin(\theta) + \cos(\theta))\mathbf{\hat{a}_y} + \mathbf{\hat{a}_z}

And if we wish to express :math:`\mathbf{a}` in the :math:`\mathbf{B}`, we do:

.. math::
  \mathbf{a} &= \mathbf{\hat{a}_x} + \mathbf{\hat{a}_y} + \mathbf{\hat{a}_z}\\
  \mathbf{a} &= \begin{bmatrix}\mathbf{\hat{b}_x}\cdot (\mathbf{\hat{a}_x} +
  \mathbf{\hat{a}_y} + \mathbf{\hat{a}_z})\end{bmatrix} \mathbf{\hat{b}_x} +
  \begin{bmatrix}\mathbf{\hat{b}_y}\cdot (\mathbf{\hat{a}_x} +
  \mathbf{\hat{a}_y} + \mathbf{\hat{a}_z})\end{bmatrix} \mathbf{\hat{b}_y} +
  \begin{bmatrix}\mathbf{\hat{b}_z}\cdot (\mathbf{\hat{a}_x} +
  \mathbf{\hat{a}_y} + \mathbf{\hat{a}_z})\end{bmatrix} \mathbf{\hat{b}_z}\\
  \mathbf{a} &= (\cos(\theta) + \sin(\theta))\mathbf{\hat{b}_x} +
  (-\sin(\theta)+\cos(\theta))\mathbf{\hat{b}_y} + \mathbf{\hat{b}_z}


Derivatives with Multiple Frames
--------------------------------

If we have reference frames :math:`\mathbf{A}` and :math:`\mathbf{B}`
we will have two sets of basis vectors. We can then define two
vectors: :math:`\mathbf{a} = a_x\mathbf{\hat{a}_x} + a_y\mathbf{\hat{a}_y} +
a_z\mathbf{\hat{a}_z}` and :math:`\mathbf{b} = b_x\mathbf{\hat{b}_x} +
b_y\mathbf{\hat{b}_y} + b_z\mathbf{\hat{b}_z}`. If we want to take the
derivative of :math:`\mathbf{b}` in the reference frame :math:`\mathbf{A}`, we
must first express it in :math:`\mathbf{A}`, and the take the derivatives of
the measure numbers:

.. math::
  \frac{^{\mathbf{A}} d\mathbf{b}}{dx} = \frac{d (\mathbf{b}\cdot
  \mathbf{\hat{a}_x} )}{dx} \mathbf{\hat{a}_x} + \frac{d (\mathbf{b}\cdot
  \mathbf{\hat{a}_y} )}{dx} \mathbf{\hat{a}_y} + \frac{d (\mathbf{b}\cdot
  \mathbf{\hat{a}_z} )}{dx} \mathbf{\hat{a}_z} +


Examples
--------

An example of vector calculus:

.. image:: vec_simp_der.*
   :height: 500
   :width: 350
   :align: center

In this example we have two bodies, each with an attached reference frame.
We will say that :math:`\theta` and :math:`x` are functions of time.
We wish to know the time derivative of vector :math:`\mathbf{c}` in both the
:math:`\mathbf{A}` and :math:`\mathbf{B}` frames.

First, we need to define :math:`\mathbf{c}`;
:math:`\mathbf{c}=x\mathbf{\hat{b}_x}+l\mathbf{\hat{b}_y}`. This provides a
definition in the :math:`\mathbf{B}` frame. We can now do the following:

.. math::
  \frac{^{\mathbf{B}} d \mathbf{c}}{dt} &= \frac{dx}{dt} \mathbf{\hat{b}_x} +
  \frac{dl}{dt} \mathbf{\hat{b}_y}\\
  &= \dot{x} \mathbf{\hat{b}_x}

To take the derivative in the :math:`\mathbf{A}` frame, we have to first relate
the two frames:

.. math::
  ^{\mathbf{A}} \mathbf{C} ^{\mathbf{B}} =
  \begin{bmatrix}
  \cos(\theta) & 0 & \sin(\theta)\\
  0 & 1 & 0\\
  -\sin(\theta) & 0 & \cos(\theta)\\
  \end{bmatrix}

Now we can do the following:

.. math::
  \frac{^{\mathbf{A}} d \mathbf{c}}{dt} &= \frac{d (\mathbf{c} \cdot
  \mathbf{\hat{a}_x})}{dt} \mathbf{\hat{a}_x} + \frac{d (\mathbf{c} \cdot
  \mathbf{\hat{a}_y})}{dt} \mathbf{\hat{a}_y} + \frac{d (\mathbf{c} \cdot
  \mathbf{\hat{a}_z})}{dt} \mathbf{\hat{a}_z}\\
  &= \frac{d (\cos(\theta) x)}{dt} \mathbf{\hat{a}_x} +
  \frac{d (l)}{dt} \mathbf{\hat{a}_y} +
  \frac{d (-\sin(\theta) x)}{dt} \mathbf{\hat{a}_z}\\
  &= (-\dot{\theta}\sin(\theta)x + \cos(\theta)\dot{x}) \mathbf{\hat{a}_x} +
  (\dot{\theta}\cos(\theta)x + \sin(\theta)\dot{x}) \mathbf{\hat{a}_z}

Note that this is the time derivative of :math:`\mathbf{c}` in
:math:`\mathbf{A}`, and is expressed in the :math:`\mathbf{A}` frame. We can
express it in the :math:`\mathbf{B}` frame however, and the expression will
still be valid:

.. math::
  \frac{^{\mathbf{A}} d \mathbf{c}}{dt} &= (-\dot{\theta}\sin(\theta)x +
  \cos(\theta)\dot{x}) \mathbf{\hat{a}_x} + (\dot{\theta}\cos(\theta)x +
  \sin(\theta)\dot{x}) \mathbf{\hat{a}_z}\\
  &= \dot{x}\mathbf{\hat{b}_x} - \theta x \mathbf{\hat{b}_z}\\

Note the difference in expression complexity between the two forms. They are
equivalent, but one is much simpler. This is an extremely important concept, as
defining vectors in the more complex forms can vastly slow down formulation of
the equations of motion and increase their length, sometimes to a point where
they cannot be shown on screen.

Using Vectors and Reference Frames
==================================

We have waited until after all of the relevant mathematical relationships have
been defined for vectors and reference frames to introduce code. This is due to
how vectors are formed. When starting any problem in :mod:`sympy.physics.vector`, one of
the first steps is defining a reference frame (remember to import
sympy.physics.vector first)::

  >>> from sympy.physics.vector import *
  >>> N = ReferenceFrame('N')

Now we have created a reference frame, :math:`\mathbf{N}`. To have access to
any basis vectors, first a reference frame needs to be created. Now that we
have made and object representing :math:`\mathbf{N}`, we can access its basis
vectors::

  >>> N.x
  N.x
  >>> N.y
  N.y
  >>> N.z
  N.z

Vector Algebra, in physics.vector
---------------------------------

We can now do basic algebraic operations on these vectors.::

  >>> N.x == N.x
  True
  >>> N.x == N.y
  False
  >>> N.x + N.y
  N.x + N.y
  >>> 2 * N.x + N.y
  2*N.x + N.y

Remember, don't add a scalar quantity to a vector (``N.x + 5``); this will
raise an error. At this point, we'll use SymPy's Symbol in our vectors.
Remember to refer to SymPy's Gotchas and Pitfalls when dealing with symbols.::

  >>> from sympy import Symbol, symbols
  >>> x = Symbol('x')
  >>> x * N.x
  x*N.x
  >>> x*(N.x + N.y)
  x*N.x + x*N.y

In :mod:`sympy.physics.vector` multiple interfaces to vector multiplication have been
implemented, at the operator level, method level, and function level. The
vector dot product can work as follows: ::

  >>> N.x & N.x
  1
  >>> N.x & N.y
  0
  >>> N.x.dot(N.x)
  1
  >>> N.x.dot(N.y)
  0
  >>> dot(N.x, N.x)
  1
  >>> dot(N.x, N.y)
  0

The "official" interface is the function interface; this is what will be used
in all examples. This is to avoid confusion with the attribute and methods
being next to each other, and in the case of the operator operation priority.
The operators used in :mod:`sympy.physics.vector` for vector multiplication do not posses
the correct order of operations; this can lead to errors. Care with parentheses
is needed when using operators to represent vector multiplication.

The cross product is the other vector multiplication which will be discussed
here. It offers similar interfaces to the dot product, and comes with the same
warnings. ::

  >>> N.x ^ N.x
  0
  >>> N.x ^ N.y
  N.z
  >>> N.x.cross(N.x)
  0
  >>> N.x.cross(N.z)
  - N.y
  >>> cross(N.x, N.y)
  N.z
  >>> N.x ^ (N.y + N.z)
  - N.y + N.z

Two additional operations can be done with vectors: normalizing the vector to
length 1, and getting its magnitude. These are done as follows::

  >>> (N.x + N.y).normalize()
  sqrt(2)/2*N.x + sqrt(2)/2*N.y
  >>> (N.x + N.y).magnitude()
  sqrt(2)

Vectors are often expressed in a matrix form, especially for numerical
purposes. Since the matrix form does not contain any information about the
reference frame the vector is defined in, you must provide a reference frame to
extract the measure numbers from the vector. There is a convenience function to
do this::

  >>> (x * N.x + 2 * x * N.y + 3 * x * N.z).to_matrix(N)
  Matrix([
    [  x],
    [2*x],
    [3*x]])

Vector Calculus, in physics.vector
----------------------------------

We have already introduced our first reference frame. We can take the
derivative in that frame right now, if we desire: ::

  >>> (x * N.x + N.y).diff(x, N)
  N.x

SymPy has a ``diff`` function, but it does not currently work with
:mod:`sympy.physics.vector` Vectors, so please use ``Vector``'s ``diff`` method.  The
reason for this is that when differentiating a ``Vector``, the frame of
reference must be specified in addition to what you are taking the derivative
with respect to; SymPy's ``diff`` function doesn't fit this mold.

The more interesting case arise with multiple reference frames. If we introduce
a second reference frame, :math:`\mathbf{A}`, we now have two frames. Note that
at this point we can add components of :math:`\mathbf{N}` and
:math:`\mathbf{A}` together, but cannot perform vector multiplication, as no
relationship between the two frames has been defined. ::

  >>> A = ReferenceFrame('A')
  >>> A.x + N.x
  N.x + A.x

If we want to do vector multiplication, first we have to define and
orientation. The ``orient`` method of ``ReferenceFrame`` provides that
functionality. ::

  >>> A.orient(N, 'Axis', [x, N.y])

If we desire, we can view the DCM between these two frames at any time. This
can be calculated with the ``dcm`` method. This code: ``N.dcm(A)`` gives the
dcm :math:`^{\mathbf{A}} \mathbf{C} ^{\mathbf{N}}`.

This orients the :math:`\mathbf{A}` frame relative to the :math:`\mathbf{N}`
frame by a simple rotation around the Y axis, by an amount x. Other, more
complicated rotation types include Body rotations, Space rotations,
quaternions, and arbitrary axis rotations. Body and space rotations are
equivalent to doing 3 simple rotations in a row, each about a basis vector in
the new frame. An example follows: ::


  >>> N = ReferenceFrame('N')
  >>> Bp = ReferenceFrame('Bp')
  >>> Bpp = ReferenceFrame('Bpp')
  >>> B = ReferenceFrame('B')
  >>> q1,q2,q3 = symbols('q1 q2 q3')
  >>> Bpp.orient(N,'Axis', [q1, N.x])
  >>> Bp.orient(Bpp,'Axis', [q2, Bpp.y])
  >>> B.orient(Bp,'Axis', [q3, Bp.z])
  >>> N.dcm(B)
  Matrix([
  [                          cos(q2)*cos(q3),                           -sin(q3)*cos(q2),          sin(q2)],
  [sin(q1)*sin(q2)*cos(q3) + sin(q3)*cos(q1), -sin(q1)*sin(q2)*sin(q3) + cos(q1)*cos(q3), -sin(q1)*cos(q2)],
  [sin(q1)*sin(q3) - sin(q2)*cos(q1)*cos(q3),  sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1),  cos(q1)*cos(q2)]])
  >>> B.orient(N,'Body',[q1,q2,q3],'XYZ')
  >>> N.dcm(B)
  Matrix([
  [                          cos(q2)*cos(q3),                           -sin(q3)*cos(q2),          sin(q2)],
  [sin(q1)*sin(q2)*cos(q3) + sin(q3)*cos(q1), -sin(q1)*sin(q2)*sin(q3) + cos(q1)*cos(q3), -sin(q1)*cos(q2)],
  [sin(q1)*sin(q3) - sin(q2)*cos(q1)*cos(q3),  sin(q1)*cos(q3) + sin(q2)*sin(q3)*cos(q1),  cos(q1)*cos(q2)]])

Space orientations are similar to body orientation, but applied from the frame
to body. Body and space rotations can involve either two or three axes: 'XYZ'
works, as does 'YZX', 'ZXZ', 'YXY', etc. What is key is that each simple
rotation is about a different axis than the previous one; 'ZZX' does not
completely orient a set of basis vectors in 3 space.

Sometimes it will be more convenient to create a new reference frame and orient
relative to an existing one in one step. The ``orientnew`` method allows for
this functionality, and essentially wraps the ``orient`` method. All of the
things you can do in ``orient``, you can do in ``orientnew``. ::

  >>> C = N.orientnew('C', 'Axis', [q1, N.x])

Quaternions (or Euler Parameters) use 4 value to characterize the orientation
of the frame. This and arbitrary axis rotations are described in the ``orient``
and ``orientnew`` method help, or in the references [Kane1983]_.


Finally, before starting multiframe calculus operations, we will introduce
another :mod:`sympy.physics.vector` tool: ``dynamicsymbols``. ``dynamicsymbols`` is
a shortcut function to create undefined functions of time within SymPy. The
derivative of such a 'dynamicsymbol' is shown below. ::

  >>> from sympy import diff
  >>> q1, q2, q3 = dynamicsymbols('q1 q2 q3')
  >>> diff(q1, Symbol('t'))
  Derivative(q1(t), t)

The 'dynamicsymbol' printing is not very clear above; we will also introduce a
few other tools here. We can use ``vprint`` instead of print for
non-interactive sessions. ::

  >>> q1
  q1(t)
  >>> q1d = diff(q1, Symbol('t'))
  >>> vprint(q1)
  q1
  >>> vprint(q1d)
  q1'

For interactive sessions use ``init_vprinting``. There also exist analogs
for SymPy's ``vprint``, ``vpprint``, and ``latex``, ``vlatex``. ::

  >>> from sympy.physics.vector import init_vprinting
  >>> init_vprinting(pretty_print=False)
  >>> q1
  q1
  >>> q1d
  q1'

A 'dynamicsymbol' should be used to represent any time varying quantity in
:mod:`sympy.physics.vector`, whether it is a coordinate, varying position, or force.  The
primary use of a 'dynamicsymbol' is for speeds and coordinates (of which there
will be more discussion in the Kinematics Section of the documentation).

Now we will define the orientation of our new frames with a 'dynamicsymbol',
and can take derivatives and time derivatives with ease. Some examples follow.
::

  >>> N = ReferenceFrame('N')
  >>> B = N.orientnew('B', 'Axis', [q1, N.x])
  >>> (B.y*q2 + B.z).diff(q2, N)
  B.y
  >>> (B.y*q2 + B.z).dt(N)
  (-q1' + q2')*B.y + q2*q1'*B.z

Note that the output vectors are kept in the same frames that they were
provided in. This remains true for vectors with components made of basis
vectors from multiple frames: ::

  >>> (B.y*q2 + B.z + q2*N.x).diff(q2, N)
  N.x + B.y


How Vectors are Coded
---------------------

What follows is a short description of how vectors are defined by the code in
:mod:`sympy.physics.vector`. It is provided for those who want to learn more about how
this part of :mod:`sympy.physics.vector` works, and does not need to be read
to use this module; don't read it unless you want to learn how this module was
implemented.

Every ``Vector``'s main information is stored in the ``args`` attribute, which
stores the three measure numbers for each basis vector in a frame, for every
relevant frame. A vector does not exist in code until a ``ReferenceFrame``
is created. At this point, the ``x``, ``y``, and ``z`` attributes of the
reference frame are immutable ``Vector``'s which have measure numbers of
[1,0,0], [0,1,0], and [0,0,1] associated with that ``ReferenceFrame``. Once
these vectors are accessible, new vectors can be created by doing algebraic
operations with the basis vectors. A vector can have components from multiple
frames though. That is why ``args`` is a list; it has as many elements in the
list as there are unique ``ReferenceFrames`` in its components, i.e. if there
are ``A`` and ``B`` frame basis vectors in our new vector, ``args`` is of
length 2; if it has ``A``, ``B``, and ``C`` frame basis vector, ``args`` is of
length three.

Each element in the ``args`` list is a 2-tuple; the first element is a SymPy
``Matrix`` (this is where the measure numbers for each set of basis vectors are
stored) and the second element is a ``ReferenceFrame`` to associate those
measure numbers with.

``ReferenceFrame`` stores a few things. First, it stores the name you supply it
on creation (``name`` attribute). It also stores the direction cosine matrices,
defined upon creation with the ``orientnew`` method, or calling the ``orient``
method after creation. The direction cosine matrices are represented by SymPy's
``Matrix``, and are part of a dictionary where the keys are the
``ReferenceFrame`` and the value the ``Matrix``; these are set
bi-directionally; in that when you orient ``A`` to ``N`` you are setting ``A``'s
orientation dictionary to include ``N`` and its ``Matrix``, but you are also
setting ``N``'s orientation dictionary to include ``A`` and its ``Matrix``
(that DCM being the transpose of the other).
