turkey3_scratch :
Not sure if anyone will ever decide to join me in this discussion (sort of lonely here haha) but anyway, I think I've realized why so many people are confused about current. Current as a noun is different than current as a measurement. Current as a noun would be a flow of charge. A flow is a noun, so a flow of charge is a noun. Only problem is, current is measured in coulombs per second, which actually refers to the amount of charge passing any cross-sectional area in a circuit per second. So current as a measurement is a rate.
So, if we say "high current" it makes sense as a rate but not as a noun. How can you have a "high flow of charge"? You can have a high "rate of flow of charge" but not a high "flow of charge". Saying current is "fast" is better terminology because it fits both contexts. A flow of charge can be fast, and the amount of coulombs passing a cross-sectional area per second can also be fast. Or the rate of flow of charge can also be fast.
Perhaps if current didn't refer to both the flow of charge and the rate of the flow of charge, people would be less confused about current and would not have misconceptions that current is a "stuff" that when it is "high" there is more of it. When a current is fast or slow there is still the same amount of "stuff" which is charge; even when there is no current, the stuff is still there. It'd be better if we completely did away with the ampere and just stuck with coulombs per second. Too many people seem to ignore charge when it comes to current, which is very bad. When we stop thinking about charge, people can't understand these concepts.
I think that you're driving yourself into confusion by attempting to frame scientific definitions in terms of language grammar. Electromagnetics is a field of science, not language arts.
Charge, measured in coulombs, is defined as the number of charges on a one farad capacitor with a potential of one volt between the plates.
Current, measured in amperes, is defined as the time rate of change of charge. It is the time-domain derivative of charge. An average of one ampere over a period of one second yields one coulomb of charge.
Current density, measured in amperes per square meter is the spatial-domain derivative of current. This is relevant to material analysis and won't be seen in a circuit topology anymore than resistivity would be seen in a circuit topology.
One thing that may confuse you a bit, and I would not be surprised if it did because it's not taught at all outside of electrical and computer engineering classes, is the relationship between the electric field and electric current.
Electrons moves very, very quickly. However, they spend the vast majority of their time zipping around the atoms to which they are bound or locally within a conductive lattice such as a metal. This natural movement is due to the thermal excitation of the material. When an electron is placed in an electric field, that field exerts a force (measured in newtons) on the electron, which causes it to have some net velocity. This net velocity is called the
drift velocity.
The drift velocity of electrons is a function of material properties and the strength of the electric field. I'll let you look up some specific examples, but I will tell you that it is very, very low. A typical drift velocity for electrons in a one ampere current through a narrow wire at low voltage is in the range of micrometers per second.
By comparison, electric fields propagate very, very quickly. In free space, the propagation rate of an electric field is C, or the speed of light. This is because the electric field modulator is the photon.
In an unshielded conductive medium such as a pair of twisted copper wires, the propagation rate is around 0.97C, or just below the speed of light. In a shielded conductive medium such as a coaxial cable, the propagation rate is around (2/3)C, or two-thirds of the speed of light.
The electric force caused by the electric field or magnetic induction causes energy to be transferred rapidly from one charge carrier to another through repulsion. Thus, while each charge carrier drifts very, very slowly, the information carried by the field propagates very, very quickly.
If you're interested in this stuff, shoot me a PM.