278 lines
7.4 KiB
Python
278 lines
7.4 KiB
Python
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from sympy.core.backend import sympify
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from sympy.physics.vector import Point
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from sympy.utilities.exceptions import SymPyDeprecationWarning
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__all__ = ['Particle']
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class Particle:
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"""A particle.
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Explanation
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===========
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Particles have a non-zero mass and lack spatial extension; they take up no
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space.
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Values need to be supplied on initialization, but can be changed later.
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Parameters
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==========
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name : str
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Name of particle
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point : Point
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A physics/mechanics Point which represents the position, velocity, and
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acceleration of this Particle
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mass : sympifyable
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A SymPy expression representing the Particle's mass
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point
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>>> from sympy import Symbol
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>>> po = Point('po')
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>>> m = Symbol('m')
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>>> pa = Particle('pa', po, m)
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>>> # Or you could change these later
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>>> pa.mass = m
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>>> pa.point = po
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"""
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def __init__(self, name, point, mass):
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if not isinstance(name, str):
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raise TypeError('Supply a valid name.')
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self._name = name
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self.mass = mass
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self.point = point
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self.potential_energy = 0
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def __str__(self):
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return self._name
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def __repr__(self):
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return self.__str__()
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@property
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def mass(self):
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"""Mass of the particle."""
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return self._mass
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@mass.setter
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def mass(self, value):
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self._mass = sympify(value)
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@property
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def point(self):
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"""Point of the particle."""
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return self._point
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@point.setter
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def point(self, p):
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if not isinstance(p, Point):
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raise TypeError("Particle point attribute must be a Point object.")
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self._point = p
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def linear_momentum(self, frame):
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"""Linear momentum of the particle.
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Explanation
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===========
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The linear momentum L, of a particle P, with respect to frame N is
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given by
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L = m * v
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where m is the mass of the particle, and v is the velocity of the
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particle in the frame N.
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Parameters
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==========
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frame : ReferenceFrame
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The frame in which linear momentum is desired.
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point, ReferenceFrame
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>>> from sympy.physics.mechanics import dynamicsymbols
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>>> from sympy.physics.vector import init_vprinting
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>>> init_vprinting(pretty_print=False)
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>>> m, v = dynamicsymbols('m v')
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>>> N = ReferenceFrame('N')
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>>> P = Point('P')
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>>> A = Particle('A', P, m)
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>>> P.set_vel(N, v * N.x)
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>>> A.linear_momentum(N)
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m*v*N.x
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"""
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return self.mass * self.point.vel(frame)
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def angular_momentum(self, point, frame):
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"""Angular momentum of the particle about the point.
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Explanation
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===========
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The angular momentum H, about some point O of a particle, P, is given
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by:
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H = r x m * v
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where r is the position vector from point O to the particle P, m is
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the mass of the particle, and v is the velocity of the particle in
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the inertial frame, N.
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Parameters
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==========
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point : Point
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The point about which angular momentum of the particle is desired.
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frame : ReferenceFrame
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The frame in which angular momentum is desired.
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point, ReferenceFrame
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>>> from sympy.physics.mechanics import dynamicsymbols
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>>> from sympy.physics.vector import init_vprinting
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>>> init_vprinting(pretty_print=False)
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>>> m, v, r = dynamicsymbols('m v r')
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>>> N = ReferenceFrame('N')
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>>> O = Point('O')
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>>> A = O.locatenew('A', r * N.x)
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>>> P = Particle('P', A, m)
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>>> P.point.set_vel(N, v * N.y)
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>>> P.angular_momentum(O, N)
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m*r*v*N.z
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"""
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return self.point.pos_from(point) ^ (self.mass * self.point.vel(frame))
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def kinetic_energy(self, frame):
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"""Kinetic energy of the particle.
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Explanation
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===========
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The kinetic energy, T, of a particle, P, is given by
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'T = 1/2 m v^2'
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where m is the mass of particle P, and v is the velocity of the
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particle in the supplied ReferenceFrame.
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Parameters
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==========
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frame : ReferenceFrame
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The Particle's velocity is typically defined with respect to
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an inertial frame but any relevant frame in which the velocity is
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known can be supplied.
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point, ReferenceFrame
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>>> from sympy import symbols
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>>> m, v, r = symbols('m v r')
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>>> N = ReferenceFrame('N')
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>>> O = Point('O')
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>>> P = Particle('P', O, m)
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>>> P.point.set_vel(N, v * N.y)
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>>> P.kinetic_energy(N)
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m*v**2/2
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"""
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return (self.mass / sympify(2) * self.point.vel(frame) &
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self.point.vel(frame))
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@property
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def potential_energy(self):
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"""The potential energy of the Particle.
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point
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>>> from sympy import symbols
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>>> m, g, h = symbols('m g h')
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>>> O = Point('O')
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>>> P = Particle('P', O, m)
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>>> P.potential_energy = m * g * h
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>>> P.potential_energy
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g*h*m
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"""
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return self._pe
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@potential_energy.setter
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def potential_energy(self, scalar):
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"""Used to set the potential energy of the Particle.
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Parameters
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==========
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scalar : Sympifyable
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The potential energy (a scalar) of the Particle.
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Examples
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========
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>>> from sympy.physics.mechanics import Particle, Point
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>>> from sympy import symbols
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>>> m, g, h = symbols('m g h')
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>>> O = Point('O')
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>>> P = Particle('P', O, m)
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>>> P.potential_energy = m * g * h
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"""
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self._pe = sympify(scalar)
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def set_potential_energy(self, scalar):
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SymPyDeprecationWarning(
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feature="Method sympy.physics.mechanics." +
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"Particle.set_potential_energy(self, scalar)",
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useinstead="property sympy.physics.mechanics." +
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"Particle.potential_energy",
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deprecated_since_version="1.5", issue=9800).warn()
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self.potential_energy = scalar
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def parallel_axis(self, point, frame):
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"""Returns an inertia dyadic of the particle with respect to another
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point and frame.
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Parameters
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==========
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point : sympy.physics.vector.Point
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The point to express the inertia dyadic about.
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frame : sympy.physics.vector.ReferenceFrame
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The reference frame used to construct the dyadic.
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Returns
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=======
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inertia : sympy.physics.vector.Dyadic
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The inertia dyadic of the particle expressed about the provided
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point and frame.
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"""
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# circular import issue
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from sympy.physics.mechanics import inertia_of_point_mass
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return inertia_of_point_mass(self.mass, self.point.pos_from(point),
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frame)
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