harmonica.magnetic_vec_to_angles#
- harmonica.magnetic_vec_to_angles(magnetic_e, magnetic_n, magnetic_u, degrees=True)[source]#
Convert magnetic field vector to magnetic field angles
Convert the 3-component magnetic vector to intensity, and inclination and declination angles.
Note
Inclination is measured positive downward from the horizontal plane and declination is measured with respect to North and it is positive east.
- Parameters:
- magnetic_e
float
orarray
Easting component of the magnetic vector.
- magnetic_n
float
orarray
Northing component of the magnetic vector.
- magnetic_u
float
orarray
Upward component of the magnetic vector.
- degreesbool (
optional
) If True, the angles are returned in degrees. If False, the angles are returned in radians. Default True.
- magnetic_e
- Returns:
- intensity:
float
orarray
Intensity of the magnetic vector.
- inclination
float
orarray
Inclination angle of the magnetic vector. If
degrees
is True, then the angle is returned in degree, else it’s returned in radians.- declination
float
orarray
Declination angle of the magnetic vector. If
degrees
is True, then the angle is returned in degrees, else it’s returned in radians.
- intensity:
Notes
The intensity of the magnetic vector is calculated as:
\[T = \sqrt{B_e^2 + B_n^2 + B_u^2}\]where \(B_e\), \(B_n\), \(B_u\) are the easting, northing and upward components of the magnetic vector, respectively.
The inclination angle is defined as the angle between the magnetic field vector and the horizontal plane:
\[I = \arctan \frac{- B_u}{\sqrt{B_e^2 + B_n^2}}\]And the declination angle is defined as the azimuth of the projection of the magnetic field vector onto the horizontal plane (starting from the northing direction, positive to the east and negative to the west):
\[D = \arcsin \frac{B_e}{\sqrt{B_e^2 + B_n^2}}\]Examples
>>> intensity, inc, dec = magnetic_vec_to_angles(1.5, 1.5, -2.12132) >>> print(intensity, inc, dec) 3.0 45.0 45.0