alfredblase
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Hi its me again, stuck once more. Sorry guys and gals :P
Ok a problem I found on http://en.wikipedia.org/wiki/Action_(physics)
In a 1-D case how do we get from:
\delta S = \int_{t_1}^{t_2} [L(x + \varepsilon, \dot{x} + \dot{\varepsilon})-L(x,\dot{x})]dt
to:
\delta S = \int_{t_1}^{t_2} \left(\varepsilon \frac{\pd L}{\pd x} + \dot{\varepsilon} \frac {\pd L} {\pd \dot{x}}\right)dt
where \varepsilon = x_1(t) - x(t)
and where the first order expansion of L in ε and ε′ is used? I don't even know what that last phrase means, so if someone could explain that to me too, that would be great.
Thankyou very much.
Ok a problem I found on http://en.wikipedia.org/wiki/Action_(physics)
In a 1-D case how do we get from:
\delta S = \int_{t_1}^{t_2} [L(x + \varepsilon, \dot{x} + \dot{\varepsilon})-L(x,\dot{x})]dt
to:
\delta S = \int_{t_1}^{t_2} \left(\varepsilon \frac{\pd L}{\pd x} + \dot{\varepsilon} \frac {\pd L} {\pd \dot{x}}\right)dt
where \varepsilon = x_1(t) - x(t)
and where the first order expansion of L in ε and ε′ is used? I don't even know what that last phrase means, so if someone could explain that to me too, that would be great.
Thankyou very much.
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