- #1
quantum_smile
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Homework Statement
My question is just about a small mathematical detail, but I'll give some context anyways.
(From Rubakov Sec. 2.2)
An expression for energy is given by
[tex] E= \int{}d^3x\frac{\delta{}L}{\delta{}\dot{\phi}(\vec{x})}\dot{\phi}(\vec{x}) - L,
[/tex]
where L is the Lagrangian,
[tex]
L=\int{}d^3{}x(\frac{1}{2}\dot{\phi}^2-\frac{1}{2}\partial_i\phi\partial_i\phi-\frac{m^2}{2}\phi^2).
[/tex]
To derive the expression for energy, Rubakov says that
[tex]
\frac{\delta{}L}{\delta{}\dot{\phi}(\vec{x})}=\dot{\phi}(\vec{x}).
[/tex]
What I want to know is, simply, how does he get this expression for
[tex]
\frac{\delta{}L}{\delta{}\dot{\phi}(\vec{x})}
[/tex]?
Homework Equations
The Attempt at a Solution
If I evaluate the expression, I just get
[tex]
\delta{}L=\int{}d^3x(\dot{\phi}).
[/tex]
Where'd the integral go in Rubakov's expression?