Chandrasekhar–Fermi method

Chandrasekhar–Fermi method or CF method or Davis–Chandrasekhar–Fermi method is a method that is used to calculate the mean strength of the interstellar magnetic field that is projected on the plane of the sky. The method was described by Subrahmanyan Chandrasekhar and Enrico Fermi in 1953[1] and independently by Leverett Davis Jr in 1951.[2] According to this method, the magnetic field in the plane of the sky is given by

where is the mass density, is the line-of-sight velocity dispersion and is the dispersion of polarization angles and is an order unity factor, which is typically taken it to be .[3][4][5] The method is also employed for prestellar molecular clouds.[6]

References

  1. Chandrasekhar, S., & Fermi, E. (1953). Magnetic Fields in Spiral Arms. The Astrophysical Journal, 118, 113.
  2. Davis Jr, L. (1951). The strength of interstellar magnetic fields. Physical Review, 81(5), 890.
  3. Heitsch, F., Zweibel, E. G., Mac Low, M. M., Li, P., & Norman, M. L. (2001). Magnetic field diagnostics based on far-infrared polarimetry: tests using numerical simulations. The Astrophysical Journal, 561(2), 800.
  4. Padoan, P., Goodman, A., Draine, B. T., Juvela, M., Nordlund, Å., & Rögnvaldsson, Ö. E. (2001). Theoretical models of polarized dust emission from protostellar cores. The Astrophysical Journal, 559(2), 1005.
  5. Ostriker, E. C., Stone, J. M., & Gammie, C. F. (2001). Density, velocity, and magnetic field structure in turbulent molecular cloud models. The Astrophysical Journal, 546(2), 980.
  6. Crutcher, R. M., Nutter, D. J., Ward-Thompson, D., & Kirk, J. M. (2004). SCUBA polarization measurements of the magnetic field strengths in the L183, L1544, and L43 prestellar cores. The Astrophysical Journal, 600(1), 279.
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