I'll add about impedance and phase.
When you look at the impedance graph, you will notice it states magnitude. Impedance is a sum of real and imaginary value. Z = R +jX. R is the real value, and X is the value of the imaginary part of the impedance Z. Impedance is a general term so if X = 0, impedance is real valued or purely resistive or resistance. If R is zero, it's purely reactive(capacitive or inductive with Z being either -jX or jX)
The magnitude value of Z is like the hypotenuse of the triangle of the impedance or the root of R^2 + X^2 which is the value at specific frequencies on the impedance response graph.
When there is a complex component X to the impedance Z, there is a phase. Or what we can visualize as current and voltage waveform not being synchronized or timed together. Since according to Ohm's law V = I*Z,. Z=V/I and can get the phase angle from converting the rectangular form of Z to phasor form using Euler's identity. With some trig you get the phase angle, and positive phase is voltage leading current.
So with this said, if the magnitude increase as frequency increases since if inductive, Z=jwL with w being frequency, and capacitance Z=1/jwC.
So, based on this, when you look at the increase in magnitude of impedance as frequency gets higher, you know the complex part of Z is inductive, and if getting lower, complex part is capacitive.
Also if complex part X of Z is negative valued, that means it's capacitive. Since for capacitor, Z=1/jwC = -j/wC
This also means that the phase will be a negative value or current leading voltage.
So, all this explains why when the magnitude of impedance increases, impedance has inductive part, and capacitive when magnitude is decreasing.
Also phase is negative when there is capacitance, and positive when there is inductance, and purely resistive when phase is zero. You can see all this on the graph below.
And with all this info, you can guess what it means when the graph looks like this.