Kerr-Newman Geometry Utilities¶
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einsteinpy.utils.kerrnewman_utils.
nonzero_christoffels_list
= [(0, 0, 1), (0, 0, 2), (0, 1, 3), (0, 2, 3), (0, 1, 0), (0, 2, 0), (0, 3, 1), (0, 3, 2), (1, 0, 0), (1, 1, 1), (1, 2, 2), (1, 3, 3), (2, 0, 0), (2, 1, 1), (2, 2, 2), (2, 3, 3), (1, 0, 3), (1, 1, 2), (2, 0, 3), (2, 1, 2), (1, 2, 1), (1, 3, 0), (2, 2, 1), (2, 3, 0), (3, 0, 1), (3, 0, 2), (3, 1, 0), (3, 1, 3), (3, 2, 0), (3, 2, 3), (3, 3, 1), (3, 3, 2)]¶ Precomputed list of tuples consisting of indices of christoffel symbols which are non-zero in Kerr-Newman Metric
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einsteinpy.utils.kerrnewman_utils.
charge_length_scale
(Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns a length scale corrosponding to the Electric Charge Q of the mass
- Parameters
- Returns
returns (coulomb’s constant^0.5)*(Q/c^2)*G^0.5
- Return type
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einsteinpy.utils.kerrnewman_utils.
rho
(r, theta, a)¶ Returns the value sqrt(r^2 + a^2 * cos^2(theta)). Specific to Boyer-Lindquist coordinates
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einsteinpy.utils.kerrnewman_utils.
delta
(r, M, a, Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns the value r^2 - Rs * r + a^2 Specific to Boyer-Lindquist coordinates
- Parameters
- Returns
The value r^2 - Rs * r + a^2 + Rq^2
- Return type
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einsteinpy.utils.kerrnewman_utils.
metric
(r, theta, M, a, Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns the Kerr-Newman Metric
- Parameters
- Returns
Numpy array of shape (4,4)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
metric_inv
(r, theta, M, a, Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns the inverse of Kerr-Newman Metric
- Parameters
- Returns
Numpy array of shape (4,4)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
dmetric_dx
(r, theta, M, a, Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns differentiation of each component of Kerr-Newman metric tensor w.r.t. t, r, theta, phi
- Parameters
- Returns
dmdx – Numpy array of shape (4,4,4) dmdx[0], dmdx[1], dmdx[2] & dmdx[3] is differentiation of metric w.r.t. t, r, theta & phi respectively
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
christoffels
(r, theta, M, a, Q, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns the 3rd rank Tensor containing Christoffel Symbols for Kerr-Newman Metric
- Parameters
- Returns
Numpy array of shape (4,4,4)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
em_potential
(r, theta, a, Q, M, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns a 4-d vector(for each component of 4-d space-time) containing the electromagnetic potential around a Kerr-Newman body
- Parameters
- Returns
Numpy array of shape (4,)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
maxwell_tensor_covariant
(r, theta, a, Q, M, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns a 2nd rank Tensor containing Maxwell Tensor with lower indices for Kerr-Newman Metric
- Parameters
- Returns
Numpy array of shape (4,4)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
maxwell_tensor_contravariant
(r, theta, a, Q, M, c=299792458.0, G=6.67408e-11, Cc=8987551787.997911)¶ Returns a 2nd rank Tensor containing Maxwell Tensor with upper indices for Kerr-Newman Metric
- Parameters
- Returns
Numpy array of shape (4,4)
- Return type
array
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einsteinpy.utils.kerrnewman_utils.
kerrnewman_time_velocity
(pos_vec, vel_vec, mass, a, Q)¶ Velocity of coordinate time wrt proper metric
- Parameters
pos_vector (array) – Vector with r, theta, phi components in SI units
vel_vector (array) – Vector with velocities of r, theta, phi components in SI units
mass (kg) – Mass of the body
a (float) – Any constant
Q (C) – Charge on the massive body
- Returns
Velocity of time
- Return type
one