I once had similar introspections about transformers, until I came across a web site,
Elliott Sound Products, which has a lot of explanation about transformers. Rod Elliott was good enough to respond to some of my questions and changed my thinking about transformers. (But don't blame him for anything I now say!)
I have done away with the idea that anything causes anything else in transformer currents. There is a mathematical relationship between primary and secondary and they can't change independently.
If the secondary current changes, perhaps a change in load resistance, so does the primary current.
If the primary current changes, perhaps a change in source resistance, so does the secondary current.
We can ascribe cause and effect, and think one changes before the other, but in reality, they change simultaneously because they are all part of one circuit.
Compare a simple series circuit with two variable resistors (and a constant voltage source.) There is a current flowing through both resistors. If you vary either one, the current changes in both of them simultaneously. Doesn't even need to be the same number of electrons in each, if we introduce a parallel resistor. The currents are now different, but still change together.
It is not the same electrons in each resistor - different electrons linked by electric field.
Just as in a transformer, different electrons in primary and secondary, linked by magnetic field.
Coming to your single inductor - bobbin, coil, choke - and the relation between emf, flux and current: again they are all mathematically related. It is no more helpful to ascribe cause and effect here. The relationship is more complex, due to the differential, but it is a mutually deterministic mathematical relation between all three.
The desciption you give from the book is much as I might describe things in a casual way. But the impression of cause and effect is misleading. It is just decribing the mathematical connection between the variables.
Lenz's law does not describe the psychology of conductors wanting to oppose changes of flux, nor the order in which changes happen. It simply says what the direction of emf IS when flux is changing.
...an external power-source brings current to the bobbin ... If current increases, so will do the magnetic flow that crosses the bobbin; therefore it will be an induced electromotive force that, according to Lenz's law, it will tend to oppose to that variation. The conclussion is a slowdown in the rate of increase of the current.
... current from a power source flows in the bobbin. If current increases, magnetic flux increases. As flux is increasing, there is an emf. Lenz says the emf is in the opposite direction to the current. At every instant that emf exactly matches the applied emf from the source. Conclusion: if you apply a constant emf to a pure inductance you get a constant rate of change of current.
The reason we may see an effect, "a slowdown in the rate of increase of the current", is dependent on the source resistance and/or on resistance of the bobbin (which can be combined.) As the current increases, IR voltage drop in the resistance increases, so the applied emf to the inductance decreases and the back emf must identically be decreasing, so the rate of change of flux must be similarly decreasing and the rate of change of current must be decreasing. All mutually deterministic.
...the induction limits the rate in which current varies.
The inductance determines the rate at which current varies, ## \frac{dI}{dt}=\frac{V}{L} ##
If I apply 10 V to a 1 H inductor, the current immediately IS increasing at 10 A/sec and continues to do so as long as I apply the 10 V. It is only the non-ideal features of the voltage source and the real inductor, that causes the limit he refers to.
It is one of the sad facts of electronic life, that all practical inductors have resitance and this is often much more significant than the similar departures from the ideal in resistors and capacitors.