Python mechanics.Point类代码示例

def test_nonminimal_pendulum():
    q1, q2 = dynamicsymbols('q1:3')
    q1d, q2d = dynamicsymbols('q1:3', level=1)
    L, m, t = symbols('L, m, t')
    g = 9.8
    # Compose World Frame
    N = ReferenceFrame('N')
    pN = Point('N*')
    pN.set_vel(N, 0)
    # Create point P, the pendulum mass
    P = pN.locatenew('P1', q1*N.x + q2*N.y)
    P.set_vel(N, P.pos_from(pN).dt(N))
    pP = Particle('pP', P, m)
    # Constraint Equations
    f_c = Matrix([q1**2 + q2**2 - L**2])
    # Calculate the lagrangian, and form the equations of motion
    Lag = Lagrangian(N, pP)
    LM = LagrangesMethod(Lag, [q1, q2], hol_coneqs=f_c,
            forcelist=[(P, m*g*N.x)], frame=N)
    LM.form_lagranges_equations()
    # Check solution
    lam1 = LM.lam_vec[0, 0]
    eom_sol = Matrix([[m*Derivative(q1, t, t) - 9.8*m + 2*lam1*q1],
                      [m*Derivative(q2, t, t) + 2*lam1*q2]])
    assert LM.eom == eom_sol
    # Check multiplier solution
    lam_sol = Matrix([(19.6*q1 + 2*q1d**2 + 2*q2d**2)/(4*q1**2/m + 4*q2**2/m)])
    assert LM.solve_multipliers(sol_type='Matrix') == lam_sol

def test_linearize_pendulum_lagrange_nonminimal():
    q1, q2 = dynamicsymbols('q1:3')
    q1d, q2d = dynamicsymbols('q1:3', level=1)
    L, m, t = symbols('L, m, t')
    g = 9.8
    # Compose World Frame
    N = ReferenceFrame('N')
    pN = Point('N*')
    pN.set_vel(N, 0)
    # A.x is along the pendulum
    theta1 = atan(q2/q1)
    A = N.orientnew('A', 'axis', [theta1, N.z])
    # Create point P, the pendulum mass
    P = pN.locatenew('P1', q1*N.x + q2*N.y)
    P.set_vel(N, P.pos_from(pN).dt(N))
    pP = Particle('pP', P, m)
    # Constraint Equations
    f_c = Matrix([q1**2 + q2**2 - L**2])
    # Calculate the lagrangian, and form the equations of motion
    Lag = Lagrangian(N, pP)
    LM = LagrangesMethod(Lag, [q1, q2], hol_coneqs=f_c, forcelist=[(P, m*g*N.x)], frame=N)
    LM.form_lagranges_equations()
    # Compose operating point
    op_point = {q1: L, q2: 0, q1d: 0, q2d: 0, q1d.diff(t): 0, q2d.diff(t): 0}
    # Solve for multiplier operating point
    lam_op = LM.solve_multipliers(op_point=op_point)
    op_point.update(lam_op)
    # Perform the Linearization
    A, B, inp_vec = LM.linearize([q2], [q2d], [q1], [q1d],
            op_point=op_point, A_and_B=True)
    assert A == Matrix([[0, 1], [-9.8/L, 0]])
    assert B == Matrix([])

def test_pendulum_angular_momentum():
    """Consider a pendulum of length OA = 2a, of mass m as a rigid body of
    center of mass G (OG = a) which turn around (O,z). The angle between the
    reference frame R and the rod is q.  The inertia of the body is I =
    (G,0,ma^2/3,ma^2/3). """

    m, a = symbols('m, a')
    q = dynamicsymbols('q')

    R = ReferenceFrame('R')
    R1 = R.orientnew('R1', 'Axis', [q, R.z])
    R1.set_ang_vel(R, q.diff() * R.z)

    I = inertia(R1, 0, m * a**2 / 3, m * a**2 / 3)

    O = Point('O')

    A = O.locatenew('A', 2*a * R1.x)
    G = O.locatenew('G', a * R1.x)

    S = RigidBody('S', G, R1, m, (I, G))

    O.set_vel(R, 0)
    A.v2pt_theory(O, R, R1)
    G.v2pt_theory(O, R, R1)

    assert (4 * m * a**2 / 3 * q.diff() * R.z -
            S.angular_momentum(O, R).express(R)) == 0

def test_partial_velocity():
    q1, q2, q3, u1, u2, u3 = dynamicsymbols("q1 q2 q3 u1 u2 u3")
    u4, u5 = dynamicsymbols("u4, u5")
    r = symbols("r")

    N = ReferenceFrame("N")
    Y = N.orientnew("Y", "Axis", [q1, N.z])
    L = Y.orientnew("L", "Axis", [q2, Y.x])
    R = L.orientnew("R", "Axis", [q3, L.y])
    R.set_ang_vel(N, u1 * L.x + u2 * L.y + u3 * L.z)

    C = Point("C")
    C.set_vel(N, u4 * L.x + u5 * (Y.z ^ L.x))
    Dmc = C.locatenew("Dmc", r * L.z)
    Dmc.v2pt_theory(C, N, R)

    vel_list = [Dmc.vel(N), C.vel(N), R.ang_vel_in(N)]
    u_list = [u1, u2, u3, u4, u5]
    assert partial_velocity(vel_list, u_list) == [
        [-r * L.y, 0, L.x],
        [r * L.x, 0, L.y],
        [0, 0, L.z],
        [L.x, L.x, 0],
        [cos(q2) * L.y - sin(q2) * L.z, cos(q2) * L.y - sin(q2) * L.z, 0],
    ]

def test_one_dof():
    # This is for a 1 dof spring-mass-damper case.
    # It is described in more detail in the Kane docstring.
    q, u = dynamicsymbols('q u')
    qd, ud = dynamicsymbols('q u', 1)
    m, c, k = symbols('m c k')
    N = ReferenceFrame('N')
    P = Point('P')
    P.set_vel(N, u * N.x)

    kd = [qd - u]
    FL = [(P, (-k * q - c * u) * N.x)]
    pa = Particle()
    pa.mass = m
    pa.point = P
    BL = [pa]

    KM = Kane(N)
    KM.coords([q])
    KM.speeds([u])
    KM.kindiffeq(kd)
    KM.kanes_equations(FL, BL)
    MM = KM.mass_matrix
    forcing = KM.forcing
    rhs = MM.inv() * forcing
    assert expand(rhs[0]) == expand(-(q * k + u * c) / m)
    assert KM.linearize() == (Matrix([[0, 1], [k, c]]), Matrix([]))

def test_one_dof():
    # This is for a 1 dof spring-mass-damper case.
    # It is described in more detail in the KanesMethod docstring.
    q, u = dynamicsymbols('q u')
    qd, ud = dynamicsymbols('q u', 1)
    m, c, k = symbols('m c k')
    N = ReferenceFrame('N')
    P = Point('P')
    P.set_vel(N, u * N.x)

    kd = [qd - u]
    FL = [(P, (-k * q - c * u) * N.x)]
    pa = Particle('pa', P, m)
    BL = [pa]

    KM = KanesMethod(N, [q], [u], kd)
    KM.kanes_equations(FL, BL)
    MM = KM.mass_matrix
    forcing = KM.forcing
    rhs = MM.inv() * forcing
    assert expand(rhs[0]) == expand(-(q * k + u * c) / m)
    assert (KM.linearize(A_and_B=True, new_method=True)[0] ==
            Matrix([[0, 1], [-k/m, -c/m]]))

    # Ensure that the old linearizer still works and that the new linearizer
    # gives the same results. The old linearizer is deprecated and should be
    # removed in >= 0.7.7.
    M_old = KM.mass_matrix_full
    # The old linearizer raises a deprecation warning, so catch it here so
    # it doesn't cause py.test to fail.
    with warnings.catch_warnings():
        warnings.filterwarnings("ignore", category=SymPyDeprecationWarning)
        F_A_old, F_B_old, r_old = KM.linearize()
    M_new, F_A_new, F_B_new, r_new = KM.linearize(new_method=True)
    assert simplify(M_new.inv() * F_A_new - M_old.inv() * F_A_old) == zeros(2)

def test_pend():
    q, u = dynamicsymbols('q u')
    qd, ud = dynamicsymbols('q u', 1)
    m, l, g = symbols('m l g')
    N = ReferenceFrame('N')
    P = Point('P')
    P.set_vel(N, -l * u * sin(q) * N.x + l * u * cos(q) * N.y)
    kd = [qd - u]

    FL = [(P, m * g * N.x)]
    pa = Particle()
    pa.mass = m
    pa.point = P
    BL = [pa]

    KM = Kane(N)
    KM.coords([q])
    KM.speeds([u])
    KM.kindiffeq(kd)
    KM.kanes_equations(FL, BL)
    MM = KM.mass_matrix
    forcing = KM.forcing
    rhs = MM.inv() * forcing
    rhs.simplify()
    assert expand(rhs[0]) == expand(-g / l * sin(q))

def test_rigidbody():
    m, m2, v1, v2, v3, omega = symbols('m m2 v1 v2 v3 omega')
    A = ReferenceFrame('A')
    A2 = ReferenceFrame('A2')
    P = Point('P')
    P2 = Point('P2')
    I = Dyadic([])
    I2 = Dyadic([])
    B = RigidBody('B', P, A, m, (I, P))
    assert B.mass == m
    assert B.frame == A
    assert B.masscenter == P
    assert B.inertia == (I, B.masscenter)

    B.mass = m2
    B.frame = A2
    B.masscenter = P2
    B.inertia = (I2, B.masscenter)
    assert B.mass == m2
    assert B.frame == A2
    assert B.masscenter == P2
    assert B.inertia == (I2, B.masscenter)
    assert B.masscenter == P2
    assert B.inertia == (I2, B.masscenter)

    # Testing linear momentum function assuming A2 is the inertial frame
    N = ReferenceFrame('N')
    P2.set_vel(N, v1 * N.x + v2 * N.y + v3 * N.z)
    assert B.linear_momentum(N) == m2 * (v1 * N.x + v2 * N.y + v3 * N.z)

def test_linearize_pendulum_lagrange_minimal():
    q1 = dynamicsymbols('q1')                     # angle of pendulum
    q1d = dynamicsymbols('q1', 1)                 # Angular velocity
    L, m, t = symbols('L, m, t')
    g = 9.8

    # Compose world frame
    N = ReferenceFrame('N')
    pN = Point('N*')
    pN.set_vel(N, 0)

    # A.x is along the pendulum
    A = N.orientnew('A', 'axis', [q1, N.z])
    A.set_ang_vel(N, q1d*N.z)

    # Locate point P relative to the origin N*
    P = pN.locatenew('P', L*A.x)
    P.v2pt_theory(pN, N, A)
    pP = Particle('pP', P, m)

    # Solve for eom with Lagranges method
    Lag = Lagrangian(N, pP)
    LM = LagrangesMethod(Lag, [q1], forcelist=[(P, m*g*N.x)], frame=N)
    LM.form_lagranges_equations()

    # Linearize
    A, B, inp_vec = LM.linearize([q1], [q1d], A_and_B=True)

    assert A == Matrix([[0, 1], [-9.8*cos(q1)/L, 0]])
    assert B == Matrix([])

def test_one_dof():
    # This is for a 1 dof spring-mass-damper case.
    # It is described in more detail in the KanesMethod docstring.
    q, u = dynamicsymbols('q u')
    qd, ud = dynamicsymbols('q u', 1)
    m, c, k = symbols('m c k')
    N = ReferenceFrame('N')
    P = Point('P')
    P.set_vel(N, u * N.x)

    kd = [qd - u]
    FL = [(P, (-k * q - c * u) * N.x)]
    pa = Particle('pa', P, m)
    BL = [pa]

    KM = KanesMethod(N, [q], [u], kd)
    # The old input format raises a deprecation warning, so catch it here so
    # it doesn't cause py.test to fail.
    with warnings.catch_warnings():
        warnings.filterwarnings("ignore", category=SymPyDeprecationWarning)
        KM.kanes_equations(FL, BL)

    MM = KM.mass_matrix
    forcing = KM.forcing
    rhs = MM.inv() * forcing
    assert expand(rhs[0]) == expand(-(q * k + u * c) / m)

    assert simplify(KM.rhs() -
                    KM.mass_matrix_full.LUsolve(KM.forcing_full)) == zeros(2, 1)

    assert (KM.linearize(A_and_B=True, )[0] == Matrix([[0, 1], [-k/m, -c/m]]))

def test_parallel_axis():
    # This is for a 2 dof inverted pendulum on a cart.
    # This tests the parallel axis code in Kane. The inertia of the pendulum is
    # defined about the hinge, not about the center of mass.

    # Defining the constants and knowns of the system
    gravity        = symbols('g')
    k, ls          = symbols('k ls')
    a, mA, mC      = symbols('a mA mC')
    F              = dynamicsymbols('F')
    Ix, Iy, Iz     = symbols('Ix Iy Iz')

    # Declaring the Generalized coordinates and speeds
    q1, q2   = dynamicsymbols('q1 q2')
    q1d, q2d = dynamicsymbols('q1 q2', 1)
    u1, u2   = dynamicsymbols('u1 u2')
    u1d, u2d = dynamicsymbols('u1 u2', 1)

    # Creating reference frames
    N = ReferenceFrame('N')
    A = ReferenceFrame('A')

    A.orient(N, 'Axis', [-q2, N.z])
    A.set_ang_vel(N, -u2 * N.z)

    # Origin of Newtonian reference frame
    O = Point('O')

    # Creating and Locating the positions of the cart, C, and the
    # center of mass of the pendulum, A
    C  = O.locatenew('C',  q1 * N.x)
    Ao = C.locatenew('Ao', a * A.y)

    # Defining velocities of the points
    O.set_vel(N, 0)
    C.set_vel(N, u1 * N.x)
    Ao.v2pt_theory(C, N, A)
    Cart     = Particle('Cart', C, mC)
    Pendulum = RigidBody('Pendulum', Ao, A, mA, (inertia(A, Ix, Iy, Iz), C))

    # kinematical differential equations

    kindiffs  = [q1d - u1, q2d - u2]

    bodyList  = [Cart, Pendulum]

    forceList = [(Ao, -N.y * gravity * mA),
                 (C,  -N.y * gravity * mC),
                 (C,  -N.x * k * (q1 - ls)),
                 (C,   N.x * F)]

    km=Kane(N)
    km.coords([q1, q2])
    km.speeds([u1, u2])
    km.kindiffeq(kindiffs)
    (fr,frstar) = km.kanes_equations(forceList, bodyList)
    mm = km.mass_matrix_full
    assert mm[3, 3] == -Iz

def test_aux():
    # Same as above, except we have 2 auxiliary speeds for the ground contact
    # point, which is known to be zero. In one case, we go through then
    # substitute the aux. speeds in at the end (they are zero, as well as their
    # derivative), in the other case, we use the built-in auxiliary speed part
    # of Kane. The equations from each should be the same.
    q1, q2, q3, u1, u2, u3  = dynamicsymbols('q1 q2 q3 u1 u2 u3')
    q1d, q2d, q3d, u1d, u2d, u3d = dynamicsymbols('q1 q2 q3 u1 u2 u3', 1)
    u4, u5, f1, f2 = dynamicsymbols('u4, u5, f1, f2')
    u4d, u5d = dynamicsymbols('u4, u5', 1)
    r, m, g = symbols('r m g')

    N = ReferenceFrame('N')
    Y = N.orientnew('Y', 'Axis', [q1, N.z])
    L = Y.orientnew('L', 'Axis', [q2, Y.x])
    R = L.orientnew('R', 'Axis', [q3, L.y])
    R.set_ang_vel(N, u1 * L.x + u2 * L.y + u3 * L.z)
    R.set_ang_acc(N, R.ang_vel_in(N).dt(R) + (R.ang_vel_in(N) ^
        R.ang_vel_in(N)))

    C = Point('C')
    C.set_vel(N, u4 * L.x + u5 * (Y.z ^ L.x))
    Dmc = C.locatenew('Dmc', r * L.z)
    Dmc.v2pt_theory(C, N, R)
    Dmc.a2pt_theory(C, N, R)

    I = inertia(L, m / 4 * r**2, m / 2 * r**2, m / 4 * r**2)

    kd = [q1d - u3/cos(q3), q2d - u1, q3d - u2 + u3 * tan(q2)]

    ForceList = [(Dmc, - m * g * Y.z), (C, f1 * L.x + f2 * (Y.z ^ L.x))]
    BodyD = RigidBody()
    BodyD.mc = Dmc
    BodyD.inertia = (I, Dmc)
    BodyD.frame = R
    BodyD.mass = m
    BodyList = [BodyD]

    KM = Kane(N)
    KM.coords([q1, q2, q3])
    KM.speeds([u1, u2, u3, u4, u5])
    KM.kindiffeq(kd)
    kdd = KM.kindiffdict()
    (fr, frstar) = KM.kanes_equations(ForceList, BodyList)
    fr = fr.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5:0})
    frstar = frstar.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5:0})

    KM2 = Kane(N)
    KM2.coords([q1, q2, q3])
    KM2.speeds([u1, u2, u3], u_auxiliary=[u4, u5])
    KM2.kindiffeq(kd)
    (fr2, frstar2) = KM2.kanes_equations(ForceList, BodyList)
    fr2 = fr2.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5:0})
    frstar2 = frstar2.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5:0})

    assert fr.expand() == fr2.expand()
    assert frstar.expand() == frstar2.expand()

def test_linear_momentum():
    N = ReferenceFrame("N")
    Ac = Point("Ac")
    Ac.set_vel(N, 25 * N.y)
    I = outer(N.x, N.x)
    A = RigidBody("A", Ac, N, 20, (I, Ac))
    P = Point("P")
    Pa = Particle("Pa", P, 1)
    Pa.point.set_vel(N, 10 * N.x)
    assert linear_momentum(N, A, Pa) == 10 * N.x + 500 * N.y

def test_aux():
    # Same as above, except we have 2 auxiliary speeds for the ground contact
    # point, which is known to be zero. In one case, we go through then
    # substitute the aux. speeds in at the end (they are zero, as well as their
    # derivative), in the other case, we use the built-in auxiliary speed part
    # of KanesMethod. The equations from each should be the same.
    q1, q2, q3, u1, u2, u3 = dynamicsymbols('q1 q2 q3 u1 u2 u3')
    q1d, q2d, q3d, u1d, u2d, u3d = dynamicsymbols('q1 q2 q3 u1 u2 u3', 1)
    u4, u5, f1, f2 = dynamicsymbols('u4, u5, f1, f2')
    u4d, u5d = dynamicsymbols('u4, u5', 1)
    r, m, g = symbols('r m g')

    N = ReferenceFrame('N')
    Y = N.orientnew('Y', 'Axis', [q1, N.z])
    L = Y.orientnew('L', 'Axis', [q2, Y.x])
    R = L.orientnew('R', 'Axis', [q3, L.y])
    w_R_N_qd = R.ang_vel_in(N)
    R.set_ang_vel(N, u1 * L.x + u2 * L.y + u3 * L.z)

    C = Point('C')
    C.set_vel(N, u4 * L.x + u5 * (Y.z ^ L.x))
    Dmc = C.locatenew('Dmc', r * L.z)
    Dmc.v2pt_theory(C, N, R)
    Dmc.a2pt_theory(C, N, R)

    I = inertia(L, m / 4 * r**2, m / 2 * r**2, m / 4 * r**2)

    kd = [dot(R.ang_vel_in(N) - w_R_N_qd, uv) for uv in L]

    ForceList = [(Dmc, - m * g * Y.z), (C, f1 * L.x + f2 * (Y.z ^ L.x))]
    BodyD = RigidBody('BodyD', Dmc, R, m, (I, Dmc))
    BodyList = [BodyD]

    KM = KanesMethod(N, q_ind=[q1, q2, q3], u_ind=[u1, u2, u3, u4, u5],
                     kd_eqs=kd)
    with warnings.catch_warnings():
        warnings.filterwarnings("ignore", category=SymPyDeprecationWarning)
        (fr, frstar) = KM.kanes_equations(ForceList, BodyList)
    fr = fr.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5: 0})
    frstar = frstar.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5: 0})

    KM2 = KanesMethod(N, q_ind=[q1, q2, q3], u_ind=[u1, u2, u3], kd_eqs=kd,
                      u_auxiliary=[u4, u5])
    with warnings.catch_warnings():
        warnings.filterwarnings("ignore", category=SymPyDeprecationWarning)
        (fr2, frstar2) = KM2.kanes_equations(ForceList, BodyList)
    fr2 = fr2.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5: 0})
    frstar2 = frstar2.subs({u4d: 0, u5d: 0}).subs({u4: 0, u5: 0})

    frstar.simplify()
    frstar2.simplify()

    assert (fr - fr2).expand() == Matrix([0, 0, 0, 0, 0])
    assert (frstar - frstar2).expand() == Matrix([0, 0, 0, 0, 0])

def test_parallel_axis():
    # This is for a 2 dof inverted pendulum on a cart.
    # This tests the parallel axis code in KanesMethod. The inertia of the
    # pendulum is defined about the hinge, not about the center of mass.

    # Defining the constants and knowns of the system
    gravity = symbols("g")
    k, ls = symbols("k ls")
    a, mA, mC = symbols("a mA mC")
    F = dynamicsymbols("F")
    Ix, Iy, Iz = symbols("Ix Iy Iz")

    # Declaring the Generalized coordinates and speeds
    q1, q2 = dynamicsymbols("q1 q2")
    q1d, q2d = dynamicsymbols("q1 q2", 1)
    u1, u2 = dynamicsymbols("u1 u2")
    u1d, u2d = dynamicsymbols("u1 u2", 1)

    # Creating reference frames
    N = ReferenceFrame("N")
    A = ReferenceFrame("A")

    A.orient(N, "Axis", [-q2, N.z])
    A.set_ang_vel(N, -u2 * N.z)

    # Origin of Newtonian reference frame
    O = Point("O")

    # Creating and Locating the positions of the cart, C, and the
    # center of mass of the pendulum, A
    C = O.locatenew("C", q1 * N.x)
    Ao = C.locatenew("Ao", a * A.y)

    # Defining velocities of the points
    O.set_vel(N, 0)
    C.set_vel(N, u1 * N.x)
    Ao.v2pt_theory(C, N, A)
    Cart = Particle("Cart", C, mC)
    Pendulum = RigidBody("Pendulum", Ao, A, mA, (inertia(A, Ix, Iy, Iz), C))

    # kinematical differential equations

    kindiffs = [q1d - u1, q2d - u2]

    bodyList = [Cart, Pendulum]

    forceList = [(Ao, -N.y * gravity * mA), (C, -N.y * gravity * mC), (C, -N.x * k * (q1 - ls)), (C, N.x * F)]

    km = KanesMethod(N, [q1, q2], [u1, u2], kindiffs)
    with warnings.catch_warnings():
        warnings.filterwarnings("ignore", category=SymPyDeprecationWarning)
        (fr, frstar) = km.kanes_equations(forceList, bodyList)
    mm = km.mass_matrix_full
    assert mm[3, 3] == Iz