Assume that the electron isoenergy surface is an ellipsoid, E(k)=\frac{h^{2},k_{1},^{2},},{2m_{1},}, +\frac{h^{2},k_{2},^{2},},{2m_{2},},+\frac{h^{2},k_{3},^{2},},{2m_{3},}, And the cosines of the external magnetic field B relative to the ellipsoid's principal axis are \alpha, \beta, \gamma.Write the quasiclassical equation of motion for the electron.

Options:
A. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\alpha -v_{3},B\beta ) \ \frac{-e},{m_{2},}, (v_{3},B\beta -v_{1},B\gamma ) \ \frac{-e},{m_{3},}, (v_{1},B\gamma -v_{2},B\alpha ) \end{bmatrix},
B. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\alpha -v_{3},B\gamma ) \ \frac{-e},{m_{2},}, (v_{3},B\gamma -v_{1},B\beta ) \ \frac{-e},{m_{3},}, (v_{1},B\beta -v_{2},B\gamma ) \end{bmatrix},
C. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\beta -v_{3},B\alpha ) \ \frac{-e},{m_{2},}, (v_{3},B\gamma -v_{1},B\beta ) \ \frac{-e},{m_{3},}, (v_{1},B\alpha -v_{2},B\gamma ) \end{bmatrix},
D. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\gamma -v_{3},B\beta ) \ \frac{-e},{m_{2},}, (v_{3},B\alpha -v_{1},B\gamma ) \ \frac{-e},{m_{3},}, (v_{1},B\beta -v_{2},B\alpha ) \end{bmatrix},
E. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\beta -v_{3},B\gamma ) \ \frac{-e},{m_{2},}, (v_{3},B\gamma -v_{1},B\alpha ) \ \frac{-e},{m_{3},}, (v_{1},B\alpha -v_{2},B\beta ) \end{bmatrix},
F. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{3},B\alpha -v_{2},B\gamma ) \ \frac{-e},{m_{2},}, (v_{1},B\gamma -v_{3},B\beta ) \ \frac{-e},{m_{3},}, (v_{2},B\beta -v_{1},B\alpha ) \end{bmatrix},
G. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\gamma -v_{3},B\alpha ) \ \frac{-e},{m_{2},}, (v_{3},B\beta -v_{1},B\gamma ) \ \frac{-e},{m_{3},}, (v_{1},B\alpha -v_{2},B\beta ) \end{bmatrix},
H. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{3},B\beta -v_{2},B\gamma ) \ \frac{-e},{m_{2},}, (v_{1},B\gamma -v_{3},B\alpha ) \ \frac{-e},{m_{3},}, (v_{2},B\alpha -v_{1},B\beta ) \end{bmatrix},
I. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{2},B\alpha -v_{3},B\gamma ) \ \frac{-e},{m_{2},}, (v_{3},B\beta -v_{1},B\alpha ) \ \frac{-e},{m_{3},}, (v_{1},B\gamma -v_{2},B\beta ) \end{bmatrix},
J. \begin{bmatrix}, \frac{dv_{1},},{dt}, \ \frac{dv_{2},},{dt}, \ \frac{dv_{3},},{dt}, \end{bmatrix}, = \begin{bmatrix}, \frac{-e},{m_{1},}, (v_{3},B\beta -v_{2},B\gamma ) \ \frac{-e},{m_{2},}, (v_{1},B\alpha -v_{3},B\gamma ) \ \frac{-e},{m_{3},}, (v_{2},B\gamma -v_{1},B\beta ) \end{bmatrix},
Answer: D