How the charge imbalance in a plasma changes with time

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The discussion focuses on the relationship between charge density and electric fields in plasma, specifically how charge imbalance evolves over time. The user introduces the net charge density and applies Maxwell's equations but finds that the resulting equations revert to the continuity equation. The key point is that the charge deviation generates an electric field, which in turn influences the behavior of the charges. The user seeks guidance on how to effectively derive the dynamics of charge imbalance in plasma. Understanding this interaction is crucial for analyzing plasma behavior in various physical contexts.
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Homework Statement
There's a neutral plasma of protons and electrons of density ##\rho##. If the number of electrons per unit volume fluctuates around its mean value by a small amount ##\delta(\mathbf{x}, t)##, show that ##\ddot{\delta} + (\rho e^2/\epsilon_0 m_e m_p) \delta = 0##.
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I put the net charge density ##\rho_q = e\delta## so that ##\nabla \cdot \mathbf{E} = e\delta / \epsilon_0##, then I tried Maxwell IV:\begin{align*}
\dot{\mathbf{E}} + c^2 \mu_0 \mathbf{J} &= 0 \overset{\mathrm{div}}{\implies} e\dot{\delta} + \nabla \cdot \mathbf{J} = 0
\end{align*}but this just gives you back the continuity eq. How to start?
 
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This is often derived with the following logic: the charge deviation causes an electric field to be produced, and then the charges respond to that electric field.
 
I want to find the solution to the integral ##\theta = \int_0^{\theta}\frac{du}{\sqrt{(c-u^2 +2u^3)}}## I can see that ##\frac{d^2u}{d\theta^2} = A +Bu+Cu^2## is a Weierstrass elliptic function, which can be generated from ##\Large(\normalsize\frac{du}{d\theta}\Large)\normalsize^2 = c-u^2 +2u^3## (A = 0, B=-1, C=3) So does this make my integral an elliptic integral? I haven't been able to find a table of integrals anywhere which contains an integral of this form so I'm a bit stuck. TerryW

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