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vk3cpu/short_antenna.html

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<!DOCTYPE html>
<html lang="en">
<head>
<meta charset="UTF-8">
<meta name="viewport" content="width=device-width, initial-scale=1.0">
<title>VK3CPU Loaded Dipole Antenna Calculator</title>
<link rel="stylesheet" href="inductor.css">
</head>
<body>
<header>Miguel <a href="mailto:vk3cpu@gmail.com">VK3CPU</a> - Loaded Dipole Antenna Calculator<br></header>
<section class="gridLayoutClass">
<div id="inductor-container" class="inductor-container" style="position: relative;">
<canvas id="inductor2D" class="inductorClass" width="350" height="350">
</canvas>
</div>
<div class="slider_container">
<div class="sliders">
<label for="frequency_slider">f:</label>
<input type="range" id="frequency_slider" min="0.0" max="5.0" value="1.0" step="0.02">
</div>
<div class="sliders">
<label for="antenna_length_slider">l:</label>
<input type="range" id="antenna_length_slider" min="0.2" max="1.0" value="1.0" step="0.01">
</div>
<div class="sliders">
<label for="inductor_distance">d:</label>
<input type="range" id="inductor_distance" min="10" max="80" value="50" step="0.5">
</div>
<div class="sliders">
<label for="conductor_diameter_slider">AWG:</label>
<input type="range" id="conductor_diameter_slider" min="0" max="40" value="20" step="1">
</div>
</div>
<div id="notes" class="notes">
<br>
<b><u>Notes:</u></b><br>
RF Inductor Calculator was developed to help users predict the RF characteristics of a single-layer solenoid-style air-core inductor. <br><br>
<u>Inputs via the slider widgets:</u>
<ul>
<li>&#8960;a : Conductor diameter slider changes AWG from 0-40. Actual diameter displayed in decimal inches.</li>
<li>&#8960;b : Coil diameter in decimal inches.</li>
<li>c/a : 'c' is the winding-to-winding distance, measured from the conductor mid-points. The 'a' is the conductor diameter, so 'c/a' is the spacing ratio. (c/a >= 1.1)
A low-value will increase the resistance due to the proximity effect.</li>
<li>N : Number of turns or windings.</li>
<li>f : The frequency of interest (MHz) for some of the calculations. Frequency dependent results are shown on the top-right.</li>
</ul>
<p>Characteristics on the left are independent of frequency, while the characteristics on the right are dependent on the selected frequency. <br><br>
Each of the graphic representations attempt to keep the relative geometry correct, without exceeding the drawing boundary. The coil diameter
relative to the conductor diameter are representative. </p>
<u>Calculated dimensions:</u>
<ul>
<li>&#8960;o : Outer coil diameter (inches) </li>
<li>&#8960;i : Inner coil diameter (inches) - corresponds to the diameter of the winding former.</li>
<li>c : Distance between windings, measured from the conductor centers (inches).</li>
<li>&#8467; : Length of the coil (inches). Equal to c x N.</li>
</ul>
<u>Calculated parameters:</u>
<ul> <b>Frequency independent:[L]</b>
<li>L : Inductance is calculated using Nagaoka's equation incorporating his 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. </li>
<li>wire : Length of wire required to wind the inductor. </li>
</ul>
<ul> <b>Frequency dependent:[R]</b> (Text goes <font color="red">RED</font> when selected frequency > SRF. Inductor model is not accurate once SRF is exceeded.)
<li>f : Selected frequency in MHz</li>
<li>&#948; : Skin depth due to skin effect (&#956;m)</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>X&#8343; : Inductive reactance at the given frequency. (&#937;) - pure inductive component, ignoring parasitic capacitance </li>
<li>Z : Complex impedance at the given frequency. (&#937;) - includes losses due to series Rac and parallel parasitic C</li>
<li>|Z| : Impedance magnitude at the given frequency. (&#937;)</li>
<li>Q : Effective Quality Factor of the inductor at the given frequency. - (|Z.im|/Z.re)</li>
</ul>
</div>
</section>
<script src="https://cdnjs.cloudflare.com/ajax/libs/mathjs/7.5.1/math.min.js"></script>
<script src="inductor.js"></script>
<script>
function awgToMm(awg) {
//
switch (awg) {
case 40: return 0.0799;
case 39: return 0.0897;
case 38: return 0.101;
case 37: return 0.113;
case 36: return 0.127;
case 35: return 0.143;
case 34: return 0.160;
case 33: return 0.180;
case 32: return 0.202;
case 31: return 0.227;
case 30: return 0.255;
case 29: return 0.286;
case 28: return 0.321;
case 27: return 0.361;
case 26: return 0.405;
case 25: return 0.455;
case 24: return 0.511;
case 23: return 0.573;
case 22: return 0.644;
case 21: return 0.723;
case 20: return 0.812;
case 19: return 0.912;
case 18: return 1.024;
case 17: return 1.150;
case 16: return 1.291;
case 15: return 1.450;
case 14: return 1.628;
case 13: return 1.828;
case 12: return 2.053;
case 11: return 2.305;
case 10: return 2.588;
case 9: return 2.906;
case 8: return 3.264;
case 7: return 3.665;
case 6: return 4.115;
case 5: return 4.621;
case 4: return 5.189;
case 3: return 5.827;
case 2: return 6.544;
case 1: return 7.348;
case 0: return 8.251;
default: return 0.0;
}
}
// Define global storage for calculated values, so we don't recalculate the same things multiple times:
var dipole = {
length_meters : 0.0,
cond_diameter_meters : 0.0,
spacing_ratio : 0.0,
loop_turns : 0.0,
frequency_hz : 0.0,
L : 0.0,
C : 0.0,
Rdc : 0.0,
SRF : 0.0,
Xl : 0.0,
Xc : 0.0,
Z : 0.0,
skin_depth : 0.0,
Rac : 0.0,
Q : 0.0
};
// Solve all the parameters, and re-draw the canvas:
function recalculate() {
// Input variables:
//dipole.length_meters = 0.001 * antenna_length_slider.value * 25.4; // Inches to mm then to m
dipole.frequency_hz = 1.8e6 * (2 ** frequency_slider.value);
dipole.length_meters = 299792458.0 * 0.95 * antenna_length_slider.value / (2.0 * dipole.frequency_hz); //
dipole.length_feet = dipole.length_meters * 3.28084;
dipole.cond_diameter_meters = 0.001 * awgToMm(40.0 - conductor_diameter_slider.value);
dipole.cond_diameter_inches = dipole.cond_diameter_meters * 39.37008;
dipole.spacing_ratio = 0.01 * inductor_distance.value;
dipole.distance_meters = inductor_distance.value * 0.005 * dipole.length_meters;
dipole.distance_feet = dipole.distance_meters * 3.28084;
// Frequency independent characteristics:
dipole.L = 0.0;
// Redraw the canvas:
//drawDesign();
}
// Specify fonts for changing parameters controlled by the sliders:
var normal_font = "12px arial";
var emphasis_font = "bold 14px arial";
const emphasis_delay = 1200;
var loop_dia_timer_handler = 0;
var loop_dia_font = normal_font;
antenna_length_slider.oninput = function() {
recalculate();
if(loop_dia_timer_handler == 0) {
loop_dia_font = emphasis_font;
loop_dia_timer_handler = setTimeout(function(){
loop_dia_font = normal_font;
drawDesign();
loop_dia_timer_handler = 0;
}, emphasis_delay);
} else {
clearTimeout(loop_dia_timer_handler);
loop_dia_timer_handler = setTimeout(function(){
loop_dia_font = normal_font;
drawDesign();
loop_dia_timer_handler = 0;
}, emphasis_delay);
}
drawDesign();
}
var cond_dia_timer_handler = 0;
var cond_dia_font = normal_font;
conductor_diameter_slider.oninput = function() {
recalculate();
if(cond_dia_timer_handler == 0) {
cond_dia_font = emphasis_font;
cond_dia_timer_handler = setTimeout(function(){
cond_dia_font = normal_font;
drawDesign();
cond_dia_timer_handler = 0;
}, emphasis_delay);
} else {
clearTimeout(cond_dia_timer_handler);
cond_dia_timer_handler = setTimeout(function(){
cond_dia_font = normal_font;
drawDesign();
cond_dia_timer_handler = 0;
}, emphasis_delay);
}
drawDesign();
}
var spacing_timer_handler = 0;
var spacing_font = normal_font;
inductor_distance.oninput = function() {
recalculate();
if(spacing_timer_handler == 0) {
spacing_font = emphasis_font;
spacing_timer_handler = setTimeout(function(){
spacing_font = normal_font;
drawDesign();
spacing_timer_handler = 0;
}, emphasis_delay);
} else {
clearTimeout(spacing_timer_handler);
spacing_timer_handler = setTimeout(function(){
spacing_font = normal_font;
drawDesign();
spacing_timer_handler = 0;
}, emphasis_delay);
}
drawDesign();
}
var frequency_timer_handler = 0;
var frequency_font = normal_font;
frequency_slider.oninput = function() {
recalculate();
if(frequency_timer_handler == 0) {
frequency_font = emphasis_font;
frequency_timer_handler = setTimeout(function(){
frequency_font = normal_font;
drawDesign();
frequency_timer_handler = 0;
}, emphasis_delay);
} else {
clearTimeout(frequency_timer_handler);
frequency_timer_handler = setTimeout(function(){
frequency_font = normal_font;
drawDesign();
frequency_timer_handler = 0;
}, emphasis_delay);
}
drawDesign();
}
window.onresize = function() {
recalculate();
drawDesign();
}
window.onorientationchange = function() {
recalculate();
drawDesign();
}
window.onbeforeprint = function() {
console.log("onbeforeprint");
drawDesign();
}
function getInductanceFromDimensions(f, A, B, D) {
// f = frequency in MHz
// A = total antenna length in feet
// B = distance from antenna center to loading coil in feet
// D = diameter of the radiator in inches
//console.log(f, A, B, D);
const t1 = Math.log((24*((234/f) - B))/D) - 1;
const t2 = (1 - (f*B)/234)**2 - 1;
const t3 = Math.log((24*(A/2 -B))/D) - 1;
const t4 = ((f*A/2 - f*B)/234)**2 - 1;
const t5 = 234/f - B;
const t6 = A/2 - B;
const k1 = 1e6 / (34*Math.PI*f);
var retval = k1 * (t1*t2/t5 - t3*t4/t6);
return retval;
}
function drawInductor(ctx, x, y, angle) {
const l1 = 15.0;
ctx.beginPath();
ctx.moveTo(x + l1*Math.cos(angle-0.25*Math.PI), y + l1*Math.sin(angle-0.25*Math.PI));
ctx.lineTo(x + l1*Math.cos(angle+0.25*Math.PI), y + l1*Math.sin(angle+0.25*Math.PI));
ctx.lineTo(x + l1*Math.cos(angle+0.75*Math.PI), y + l1*Math.sin(angle+0.75*Math.PI));
ctx.lineTo(x + l1*Math.cos(angle+1.25*Math.PI), y + l1*Math.sin(angle+1.25*Math.PI));
ctx.lineTo(x + l1*Math.cos(angle-0.25*Math.PI), y + l1*Math.sin(angle-0.25*Math.PI));
ctx.stroke();
}
function drawArrow(ctx, x, y, angle) {
const l1 = 15.0;
const l2 = 20.0;
ctx.beginPath();
ctx.moveTo(x , y);
ctx.lineTo(x + l1*Math.cos(angle+0.33*Math.PI), y + l1*Math.sin(angle+0.33*Math.PI));
ctx.lineTo(x + l1*Math.cos(angle+0.67*Math.PI), y + l1*Math.sin(angle+0.67*Math.PI));
ctx.lineTo(x, y);
ctx.lineTo(x + l2*Math.cos(angle+0.5*Math.PI), y + l2*Math.sin(angle+0.5*Math.PI));
ctx.stroke();
}
const afront_canvas = document.getElementById("inductor2D");
const fctx = afront_canvas.getContext('2d');
function drawDesign() {
const win_width = document.getElementById("inductor-container").clientWidth;
const win_height = document.getElementById("inductor-container").clientHeight;
afront_canvas.width = win_width-12;
afront_canvas.height = win_height-12;
fctx.clearRect(0, 0, win_width, win_height);
const loopx = win_width/2;
const loopy = win_height/4;
const cond_diameter_mm = dipole.cond_diameter_meters * 1000.0;
const cond_diameter_inches = cond_diameter_mm / 25.4;
fctx.font = "bold 14px arial";
fctx.textAlign = "center";
fctx.fillText("Wire : " + (40-conductor_diameter_slider.value).toString() + "AWG : " +
"\u2300 = " + cond_diameter_inches.toFixed(4).toString() + "\" " +
"(" + cond_diameter_mm.toFixed(3).toString() + " mm)", loopx, 16);
const wire_x = win_width * 0.50;
const up_wire_top_y = win_height * 0.1;
const up_wire_bot_y = win_height * 0.5 - 5;
const down_wire_top_y = win_height * 0.5 + 5;
const down_wire_bot_y = win_height * 0.9;
var arrow_size = 10.0;
const Xl = getInductanceFromDimensions(dipole.frequency_hz * 1e-6,
dipole.length_feet,
dipole.distance_feet,
dipole.cond_diameter_inches);
//console.log(Xl);
// Draw the top antenna element:
fctx.beginPath();
fctx.moveTo(wire_x, up_wire_top_y);
fctx.lineTo(wire_x, up_wire_bot_y);
fctx.lineTo(wire_x - 15, up_wire_bot_y);
fctx.stroke();
const d_pos = up_wire_bot_y - dipole.spacing_ratio * (up_wire_bot_y - up_wire_top_y);
fctx.textAlign = "right";
drawInductor(fctx, wire_x, d_pos, 0.0*Math.PI);
drawArrow(fctx, wire_x - 30, d_pos, 0.5*Math.PI);
fctx.fillText(dipole.distance_meters.toFixed(2).toString() + " m", wire_x - 60, d_pos + 12 );
fctx.fillText(dipole.distance_feet.toFixed(2).toString() + " ft", wire_x - 60, d_pos - 4);
drawArrow(fctx, wire_x - 30, up_wire_bot_y, 0.5*Math.PI);
fctx.fillText("0.00", wire_x - 60, up_wire_bot_y + 5);
//fctx.fillText("0.00 m", wire_x - 60, up_wire_bot_y + 18);
drawArrow(fctx, wire_x - 30, up_wire_top_y, 0.5*Math.PI);
fctx.fillText((dipole.length_feet * 0.5).toFixed(2).toString() + " ft", wire_x - 60, up_wire_top_y - 4);
fctx.fillText((dipole.length_meters * 0.5).toFixed(2).toString() + " m", wire_x - 60, up_wire_top_y + 12);
fctx.textAlign = "left";
fctx.fillText(dipole.length_feet.toFixed(2).toString() + " ft", wire_x + 60, up_wire_top_y - 4);
fctx.fillText(dipole.length_meters.toFixed(2).toString() + " m", wire_x + 60, up_wire_top_y + 12);
//fctx.fillText("0.00 ft", wire_x + 60, down_wire_bot_y );
fctx.fillText("0.00", wire_x + 60, down_wire_bot_y + 5);
//drawArrow(fctx, wire_x + 10, up_wire_bot_y, -0.5*Math.PI);
const L = Xl / (2 * Math.PI * dipole.frequency_hz * 0.000001);
fctx.fillText("L = " + L.toFixed(1).toString() + " \u00B5H", wire_x + 20, d_pos - 4);
fctx.fillText("X = " + Xl.toFixed(1).toString() + " \u03A9", wire_x + 20, d_pos + 12);
fctx.font = frequency_font;
fctx.fillText("f = " + (dipole.frequency_hz * 1e-6).toFixed(2).toString() + " MHz", 20, down_wire_bot_y - 36);
fctx.font = loop_dia_font;
fctx.fillText("l = " + (antenna_length_slider.value * 1e2).toFixed(2).toString() + " %", 20, down_wire_bot_y - 18);
fctx.font = spacing_font;
fctx.fillText("d = " + (dipole.spacing_ratio * 1e2).toFixed(2).toString() + " %", 20, down_wire_bot_y );
fctx.font = cond_dia_font;
//fctx.textAlign = "center";
//fctx.fillText("f = " + (dipole.frequency_hz * 1e-6).toFixed(2).toString() + " MHz", wire_x, down_wire_bot_y + 30);
// Draw the bottom antenna element:
fctx.beginPath();
fctx.moveTo(wire_x - 15, down_wire_top_y);
fctx.lineTo(wire_x, down_wire_top_y);
fctx.lineTo(wire_x, down_wire_bot_y);
fctx.stroke();
drawInductor(fctx, wire_x, down_wire_top_y + dipole.spacing_ratio * (up_wire_bot_y - up_wire_top_y), 0.0*Math.PI);
//drawArrow(fctx, wire_x + 10, down_wire_top_y, -0.5*Math.PI);
drawArrow(fctx, wire_x + 30, down_wire_bot_y, -0.5*Math.PI);
drawArrow(fctx, wire_x + 30, up_wire_top_y, -0.5*Math.PI);
}
recalculate();
drawDesign();
</script>
</body>
</html>
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