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--- equations:hamilton-jacobi_equation [2017/11/10 16:35]
jakobadmin created
+++ equations:hamilton-jacobi_equation [2018/05/05 12:29] (current)
63.143.42.253 ↷ Links adapted because of a move operation
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 ====== Hamilton-Jacobi Equation ======
-<tabbox Why is it interesting?>
-<tabbox Layman>
+<tabbox Intuitive>
 <note tip>
@@ Line 9: / Line 9: @@
 </note>
-<tabbox Student>
+<tabbox Concrete>
 For a very nice explanation of the origin of the Hamilton-Jacobi equation and its meaning see chapter 2 in Sleeping Beauties in Theoretical Physics by Thanu Padmanabhan
-<tabbox Researcher>
-<note tip>
+<blockquote>The Hamilton-Jacobi equation is essentially a dispersion relation for
-The motto in this section is: //the higher the level of abstraction, the better//.
+a complex wave. This is easy to see in the context of non-relativistic
-</note>
+[[theories:quantum_mechanics:canonical|quantum mechanics]]. If a quantum amplitude is expressed in the
+form ψ = Rexp(iS/h¯), then the Hamilton-Jacobi equation relates
+p = ∂S/∂q to E = −∂S/∂t by the condition p2(q) = 2m(E −V).
+This is a relation between the wave vector k = p/h¯ and the frequency
+ω = E/h¯ of the “matter wave” associated with the particle.<cite>chapter 2 in Sleeping Beauties in Theoretical Physics by Thanu Padmanabhan
+</cite></blockquote>
+----
-<tabbox Examples>
---> Example1#
+Take note that while the Hamilton equation for time-evolution is closely related to the Heisenberg equation in quantum mechanics, the Hamilton-Jacobi equation is closely connected to the [[equations:schroedinger_equation|Schrödinger equation]]. See, for example, Section 4.8.1 in [[http://www.damtp.cam.ac.uk/user/tong/dynamics/four.pdf|Tong's lecture notes]].
-<--
---> Example2:#
+<tabbox Abstract>
+We consider a manifold $Q$ and a Lagrangian $L \colon TQ\rightarrow\mathbb{R}$. Now, we define Hamilton's principal function
-<--
+\[
+ W \colon Q\times\mathbb{R}\times Q\times\mathbb{R}\longrightarrow\mathbb{R}
+\]
+by
+\[
+ W(q_0,t_0; q_1, t_1) = \inf_{q\in\Upsilon} S(q)
+\]
+where
+\[
+ \Upsilon=\bigl\{ q \colon [t_0,t_1]\rightarrow Q,\, q(t_0)=q_0,\text{ \& }q(t_1)=q_1 \bigr\}
+\]
+and
+\[
+ S(q) = \int_{t_0}^{t_1} L\Bigl(q(t),\dot{q}(t)\Bigr)\,dt .
+\]
+Here $W$ is the least action for some path from $(q_0,t_0)$ to $(q_1,t_1)$. We have
+\[
+ \frac{\partial}{\partial q_1^i}W(q_0,q_1) = (p_1)_i,
+\]
+where $p_1$ is the momentum of the particle going from $q_0$ to $q_1$, at time $t_1$, and
+$$  \frac{\partial W}{\partial q_0^i}= -(p_0)_i ,\qquad\text{(-momentum at time $t_0$)} $$
+$$ \frac{\partial W}{\partial t_1}= -H_1,\qquad\text{(-energy at time $t_1$)} $$
+$$ \frac{\partial W}{\partial t_0}= H_0,\qquad\text{(+energy at time $t_0$)}
+ $$
+Take note that $H_1=H_0$ since energy is conserved.  These last four equations are the Hamilton--Jacobi equations.
-<tabbox FAQ>
-<tabbox History>
+<tabbox Why is it interesting?>
 </tabbox>

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