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Update inductor.html

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miguel 2020-11-19 07:19:48 +11:00
rodzic 628bb137a5
commit 36c74c6392
1 zmienionych plików z 4 dodań i 3 usunięć
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inductor.html
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@ -62,8 +62,9 @@
<li>L : Inductance is calculated using an equation incorporating the Nagaoka coefficient.</li>
<li>C : Capacitance is calculated using Knight's 2016 paper on self-resonance and self-capacitance of solenoid coils.</li>
<li>Rdc : DC resistance is calculated using conductor length divided by the conductor cross-sectional area, assuming a copper conductor.</li>
<li>SRF : Self-resonant frequency (MHz) for the unloaded coil. Due to the conductor length and velocity factor as described by Knight (2016).</li>
<li>X : Reactance at the given frequency. (&#937)</li>
<li>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).</li>
<li>Xl : Inductive reactance at the given frequency. (&#937)</li>
<li>&#948 : Skin depth due to skin effect (&#956m)</li>
<li>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.</li>
<li>Q : Quality factor of device, based on reactance (X) &#247 resistance (Rac) at the given frequency.</li>
@ -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);