1657 |
|
\] |
1658 |
|
, we obtain |
1659 |
|
\begin{eqnarray*} |
1660 |
< |
m\ddot x & = & - \frac{{\partial W(x)}}{{\partial x}} - |
1660 |
> |
m\ddot x & = & - \frac{{\partial W(x)}}{{\partial x}} - |
1661 |
|
\sum\limits_{\alpha = 1}^N {\left\{ {\left( { - \frac{{g_\alpha ^2 |
1662 |
|
}}{{m_\alpha \omega _\alpha ^2 }}} \right)\int_0^t {\cos (\omega |
1663 |
< |
_\alpha t)\dot x(t - \tau )d\tau \\ |
1664 |
< |
& &\mbox{} - \left[ {g_\alpha x_\alpha (0) - \frac{{g_\alpha |
1665 |
< |
}}{{m_\alpha \omega _\alpha }}} \right]\cos (\omega _\alpha t) - |
1666 |
< |
\frac{{g_\alpha \dot x_\alpha (0)}}{{\omega |
1667 |
< |
_\alpha }}\sin (\omega _\alpha t)} } \right\}} \\ |
1668 |
< |
% |
1669 |
< |
& = & - \frac{{\partial W(x)}}{{\partial x}} - \int_0^t |
1663 |
> |
_\alpha t)\dot x(t - \tau )d\tau } } \right\}} \\ |
1664 |
> |
& & + \sum\limits_{\alpha = 1}^N {\left\{ {\left[ {g_\alpha |
1665 |
> |
x_\alpha (0) - \frac{{g_\alpha }}{{m_\alpha \omega _\alpha }}} |
1666 |
> |
\right]\cos (\omega _\alpha t) + \frac{{g_\alpha \dot x_\alpha |
1667 |
> |
(0)}}{{\omega _\alpha }}\sin (\omega _\alpha t)} \right\}} |
1668 |
> |
\end{eqnarray*} |
1669 |
> |
\begin{eqnarray*} |
1670 |
> |
m\ddot x & = & - \frac{{\partial W(x)}}{{\partial x}} - \int_0^t |
1671 |
|
{\sum\limits_{\alpha = 1}^N {\left( { - \frac{{g_\alpha ^2 |
1672 |
|
}}{{m_\alpha \omega _\alpha ^2 }}} \right)\cos (\omega _\alpha |
1673 |
< |
t)\dot x(t - \tau )d} \tau } + \sum\limits_{\alpha = 1}^N {\left\{ |
1674 |
< |
{\left[ {g_\alpha x_\alpha (0) \\ |
1675 |
< |
& & \mbox{} - \frac{{g_\alpha }}{{m_\alpha \omega _\alpha }}} |
1673 |
> |
t)\dot x(t - \tau )d} \tau } \\ |
1674 |
> |
& & + \sum\limits_{\alpha = 1}^N {\left\{ {\left[ {g_\alpha |
1675 |
> |
x_\alpha (0) - \frac{{g_\alpha }}{{m_\alpha \omega _\alpha }}} |
1676 |
|
\right]\cos (\omega _\alpha t) + \frac{{g_\alpha \dot x_\alpha |
1677 |
|
(0)}}{{\omega _\alpha }}\sin (\omega _\alpha t)} \right\}} |
1678 |
|
\end{eqnarray*} |