Gauss's Law: Understanding kQ/r^2 in Point Charge Surroundings

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In the discussion on Gauss's Law, the focus is on understanding the formula kQ/r^2 in relation to a point charge and its electric field. The electric field E is constant on a Gaussian sphere surrounding the charge because all points on the sphere are equidistant from the charge. The formula indicates that the electric field strength decreases with the square of the distance from the charge, reflecting how field lines spread out. The density of these field lines correlates with the strength of the electric field, emphasizing that the field is a result of all field lines emanating from the charge, not just a single line. Overall, kQ/r^2 effectively describes the behavior of the electric field in three-dimensional space around a point charge.
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Consider a point charge surrounded by a gaussian sphere. In the derivation of the formula, we said that E is constant everywhere on the sphere. Hence, we used Flux= EA.. However, isn't the E created on the surface is due to one field line out of the pint charge. I mean the formula kQ/r^2 is the field of the charge in a particular direction? I need clarification in this. Here, i just want to know kq/r^2.. What does it respond to?
 
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ehabmozart said:
However, isn't the E created on the surface is due to one field line out of the pint charge.
Field lines are just an aid to visualizing the field. The field exists everywhere.
I mean the formula kQ/r^2 is the field of the charge in a particular direction?
That tells you the field surrounding a point charge, which depends only on the distance r from the charge. The direction of the field is radially outward (for a positive charge).
 
The field due to the point charge is constant on the surrounding sphere because every point on that sphere is at the same distance away from the charge. You can think of r^2 as the (squared) distance from the point where the charge is to wherever you're measuring the field. Every point on the sphere has the same value of r^2 so E has the same magnitude at every point on that sphere.
 
yeah, I agree with these dudes. Another point: the kq/r^2 you can think of as a consequence of how the field lines are spreading out. The 'closeness' of the field lines is proportional to the strength of the electric field. And since the field lines are spreading out as 1/r^2 , then the electric field also weakens as 1/r^2. So in this way, you can think of the electric field as due to all the field lines coming out of the point charge, not due to any single field line.
 
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