NB76
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I am sorry, I just don't see it (get it).haruspex said:What I wrote gives you a way to relate the potential of the disc to its charge density.
The discussion revolves around the equations of motion for an electron emitted from a surface, considering various geometries such as an infinite plane or a finite plate. Participants explore the implications of the electric field produced by these surfaces and how it affects the electron's trajectory, with a focus on both theoretical and practical aspects relevant to real-world applications.
Participants do not reach a consensus on the best approach to model the electron's motion. Multiple competing views exist regarding the validity of the infinite plane approximation and the necessary conditions for accurate calculations.
Limitations include the need for more information about the system, such as the charge density on the plate and the gradient of the potential. The discussion highlights the complexity of the problem and the dependence on specific parameters that have not been fully defined.
This discussion may be of interest to those working in fields related to electromagnetism, particle physics, or anyone involved in experimental setups involving electron emissions and electric fields.
I am sorry, I just don't see it (get it).haruspex said:What I wrote gives you a way to relate the potential of the disc to its charge density.
##V(x)=2\pi \sigma k(\sqrt{R^2+x^2}-x)\approx 2\pi \sigma kR(1-\frac xR)=2\frac{Qk}R(1-\frac xR)=V_0(1-\frac xR)##.NB76 said:I am sorry, I just don't see it (get it).