diff --git a/inductor.html b/inductor.html
index 15817b6..02850d7 100644
--- a/inductor.html
+++ b/inductor.html
@@ -62,8 +62,9 @@
L : Inductance is calculated using an equation incorporating the Nagaoka coefficient.
C : Capacitance is calculated using Knight's 2016 paper on self-resonance and self-capacitance of solenoid coils.
Rdc : DC resistance is calculated using conductor length divided by the conductor cross-sectional area, assuming a copper conductor.
- SRF : Self-resonant frequency (MHz) for the unloaded coil. Due to the conductor length and velocity factor as described by Knight (2016).
- X : Reactance at the given frequency. (Ω)
+ SRF : Self-resonant frequency (MHz) for the unloaded coil. Currently using a lumped reactances model. (Looking into modifying the model to
+ use the conductor length and velocity factor as described by Knight (2016).
+ Xl : Inductive reactance at the given frequency. (Ω)
δ : Skin depth due to skin effect (μm)
Rac : AC resistance is calculated using the skin effect and proximity resistance from empirical data collected by Medhurst using the spacing ratio, and length-to-diameter ratio.
Q : Quality factor of device, based on reactance (X) ÷ resistance (Rac) at the given frequency.
@@ -558,7 +559,7 @@
fctx.textAlign = "right";
var freq = 1.0 * frequency_slider.value;
fctx.fillText("f = " + freq.toFixed(1) + " MHz", win_width-18, 18);
- fctx.fillText("X = " + inductiveReactance(freq * 1e6).toFixed(1) + " \u03A9", win_width-18, 32);
+ fctx.fillText("Xl = " + inductiveReactance(freq * 1e6).toFixed(1) + " \u03A9", win_width-18, 32);
fctx.fillText("\u03B4 = " + (skinDepth() * 1e6).toFixed(1) + " \u03BCm", win_width-18, 46);
fctx.fillText("Rac = " + acResistance(freq * 1e6).toFixed(2) + " \u03A9", win_width-18, 60);
fctx.fillText("Q = " + qualityFactor(freq * 1e6).toFixed(1), win_width-18, 74);