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\samepage \begin{equation}\frac {d\omega}{dt}=F(\omega)+\Phi(t)
 \end{equation}
}

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\samepage \begin{displaymath}F(\omega )\cdot I=\left\{
 \begin{array}{rcl}
 & \dot{M}\eta _k \Omega R_G^2  - k_t\frac {\mu ^2}{R_c^3},
 \qquad  \hbox{\rm wind  accretion}\\ 
 & \dot{M}\sqrt{GMR_d}-k_t\frac {\mu ^2}{R_c^3},
 \qquad \hbox{\rm accretion disk},\\ 
 \end{array}
 \right.
\end{displaymath}
}

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\samepage \begin{equation}\frac { df}{ dt}= \frac { df \, F(\omega)}{ d\omega}+
   D \frac {d^2\, f } {d\omega^2},
 \end{equation}
}

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\samepage \begin{equation}< \Phi(t)\Phi(t') > = 2{\it D}\delta(t-t')
 \end{equation}
}

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\samepage \begin{equation}{ f}(\omega)=N\exp {(-V(\omega)/{ D})}
 \end{equation}
}

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\samepage \begin{equation}\int_{-\infty}^{\infty} {f}(\omega) \, d\omega=1
 \end{equation}
}

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\samepage \begin{equation}{ D}=\frac {k_t\mu^2}{3GMI}\cdot \frac{\omega^3}{\gamma}
 \end{equation}
}

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\samepage \begin{equation}\Delta t \approx 1.7\cdot 10^{4} \alpha^{-2}10^{2(A+8.5)}L_{37}^
 {-\frac {12}{7}}\mu_{30}^{-\frac {4}{7}} sec,
 \end{equation}
}

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\samepage \begin{equation}{D}=5.55\cdot 10^{-19}\mu _{30}^2\omega ^3
 \gamma _6^{-1}I_{45}^{-1}\left(\frac M{1.5M_{\odot}}\right)^{-1}\, s^{-3} \, .
 \end{equation}
}

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\samepage \begin{equation}D=\omega_{char} \dot{\omega}\, ,
\end{equation}
}

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\samepage \begin{equation}t_{char}=\omega_{char}/\dot{\omega} =\frac {Dp^4}{4\pi ^2 \dot{p}^2}
\end{equation}
}

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\samepage \begin{equation}\frac {R_G}{v_{sw}}=400\left(\frac M{1.5M_\odot}\right)
  \left(\frac {v_{sw}}{10^8cm/s}\right)^{-3}\qquad  sec
\end{equation}
}

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\samepage \begin{table*}
\begin{tabular}{|l|c|c|c|c|c|c|}
          &$\Delta t,\, sec$&$\gamma  $     &$D,\, sec^{-3}$    &$v_{sw},\,
km/s,\,
 $&$v_{sw},\, km/s,\, $&$t_{char},\, sec$\\ 
 &  &  &  & $(v_t=0.1a_s)$ & $(v_t=a_s)$ &  \\ 
Vela X--1 &$1.5\cdot 10^4$  &$6.3\cdot 10^6$&$8.7\cdot 10^{-24}$&$848$ &$1442$
&$200$\\ 
GX 301--2 &$1.1\cdot 10^3$  &$2.9\cdot 10^6$&$2  \cdot 10^{-21}$&$656$ &$1120$
&$245$\\ 
Her X--1  &$4\cdot 10^3  $  &$6.0\cdot 10^7$&$4  \cdot 10^{-19}$&---   &---
&$960$\\ 
Cen X--3  &$2\cdot 10^4  $  &$9.5\cdot 10^5$&$4.1\cdot 10^{-17}$&---   &---
&$8500$\\ 
\\ 
\end{tabular}
\end{table*}
}

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\samepage \begin{displaymath}\left(\frac {\dot{M}\, v_t\, R_t}{I}\right)
\end{displaymath}
}

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\samepage \begin{equation}{D}=\frac 12 \left(\frac {\dot{M}\, v_t\, R_t}{I}\right)^2\frac {R_G}{v_{sw}},
 \end{equation}
}

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\clearpage
\samepage \begin{equation}R_t\approx R_G=\frac {2GM}{v_{sw}^2}\approx 4\cdot 10^{10}v_8^{-2}\,
 \left(\frac M{1.5\, M_\odot}\right) cm,
 \end{equation}
}

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\samepage \begin{equation}v_t=\eta \cdot a_s,\qquad \eta \le 1
 \end{equation}
}

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\samepage \begin{equation}{D}=4.38\cdot 10^{-23}\dot{M} _{16}^2\eta ^2T_4\mu ^{-1}v_8^{-7}
 I_{45}^{-2}\left(\frac M{1.5\, M_\odot }\right)\, s^{-3}\, ,
 \end{equation}
}

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\samepage \setbox\sizebox=\hbox{$\dot{M} =\frac {\dot{M}}{10^{16}\, g/s},\ \ I_{45}=\frac I{10^{45}\,
 g\cdot cm^2}.$}\lthtmltypeout{latex2htmlSize :tex2html_wrap_inline632: \the\ht\sizebox::\the\dp\sizebox.}\box\sizebox
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\samepage \begin{equation}\begin{array}{rcl}
 & v_{sw}=1700\cdot D_{-24}^{-1/7}\dot{M} _{16}^{2/7}\eta ^{2/7}T_4^{1/7}
 \mu ^{-1/7}\\ 
 & I_{45}^{-2/7}\left(\frac M{1.5\, M_\odot }\right)^{2/7} \, km/s.\\ 
 \end{array}
 \end{equation}
}

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\samepage \begin{equation}v_{\infty} \approx 3\cdot v_{esc},
 \end{equation}
}

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\samepage \begin{equation}v(r)=V_{\infty} (1-\frac {R_*}r)^{\alpha}
 \end{equation}
}

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