Microstrip Calculator

Microstrip Calculator: Calculate Impedance & Wavelength :root { –primary-color: #004a99; –success-color: #28a745; –background-color: #f8f9fa; –text-color: #333; –border-color: #ddd; –card-background: #fff; –shadow: 0 4px 8px rgba(0,0,0,0.1); } body { font-family: 'Segoe UI', Tahoma, Geneva, Verdana, sans-serif; background-color: var(–background-color); color: var(–text-color); line-height: 1.6; margin: 0; padding: 0; } .container { max-width: 1000px; margin: 20px auto; padding: 20px; background-color: var(–card-background); border-radius: 8px; box-shadow: var(–shadow); } header { background-color: var(–primary-color); color: white; padding: 20px 0; text-align: center; margin-bottom: 20px; border-radius: 8px 8px 0 0; } header h1 { margin: 0; font-size: 2.2em; } .calculator-section { margin-bottom: 30px; padding: 25px; border: 1px solid var(–border-color); border-radius: 8px; background-color: var(–card-background); box-shadow: var(–shadow); } .calculator-section h2 { color: var(–primary-color); 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Microstrip Calculator

Calculate Key Parameters for Your PCB Designs

Microstrip Parameters Calculator

Height of the dielectric substrate (mm).
Width of the microstrip trace (mm).
Thickness of the conductive trace (mm).
Relative permittivity of the substrate material.
Operating frequency (GHz).

Calculation Results

Impedance: Ω Characteristic Impedance (Z0)
Effective Dielectric Constant (εeff):
Guided Wavelength (λg): mm
Trace Width to Height Ratio (w/h):
Trace Width (w): mm
Substrate Height (h): mm
Formula Used (Simplified Wheeler's Incremental Inductance Rule Approximation):

The characteristic impedance (Z0) is calculated based on the trace width (w), substrate height (h), dielectric constant (εr), and trace thickness (t). The effective dielectric constant (εeff) influences the guided wavelength (λg). These formulas are approximations valid for typical microstrip dimensions.

Z0 ≈ (60 / sqrt(εeff)) * ln(8*h/w + w/(4*h)) for w/h < 1
Z0 ≈ (120 * π / sqrt(εeff)) / (w/h + 1.393 + 0.667 * ln(h/w + 1.444)) for w/h > 1
εeff ≈ (εr + 1)/2 + (εr – 1)/2 * (1 + 12*h/w)^(-0.5) for w/h < 1
εeff ≈ (εr + 1)/2 + (εr – 1)/2 * (1 + 12*h/w)^(-0.5) for w/h > 1 (simplified, often used)
λg = λ0 / sqrt(εeff) where λ0 = c / (f * 1e9) (c is speed of light)

Microstrip Parameter Summary
Parameter Value Unit
Characteristic Impedance (Z0) Ω
Effective Dielectric Constant (εeff)
Guided Wavelength (λg) mm
Trace Width to Height Ratio (w/h)
Substrate Height (h) mm
Trace Width (w) mm
Trace Thickness (t) mm
Dielectric Constant (εr)
Frequency (f) GHz
Impedance vs. Trace Width to Height Ratio

What is a Microstrip Calculator?

A microstrip calculator is an essential online tool designed for electrical engineers, PCB designers, and RF engineers. It allows for the rapid and accurate calculation of critical parameters associated with microstrip transmission lines. Microstrip lines are fundamental components in high-frequency printed circuit boards (PCBs), acting as waveguides for electromagnetic signals. This calculator helps determine properties like characteristic impedance (Z0), effective dielectric constant (εeff), and guided wavelength (λg) based on physical dimensions and material properties. Understanding these parameters is crucial for impedance matching, signal integrity, and overall performance of RF circuits.

Who should use it? Anyone involved in the design and analysis of RF and microwave circuits on PCBs will find a microstrip calculator invaluable. This includes:

  • PCB Designers
  • RF Engineers
  • Microwave Engineers
  • Electrical Engineers
  • Students studying electromagnetics and RF design

Common Misconceptions:

  • Microstrip is lossless: While often approximated as lossless in basic calculations, real microstrip lines have conductor and dielectric losses that become significant at higher frequencies.
  • Formulas are exact: The formulas used in most calculators are approximations (like Wheeler's, Hammerstad's, or Kirschning's methods) derived from empirical data and analytical models. They provide excellent accuracy for typical design ranges but may deviate for extreme aspect ratios or materials.
  • εr is constant: The dielectric constant can vary slightly with frequency and temperature, though for many applications, a nominal value is sufficient.

Microstrip Calculator Formula and Mathematical Explanation

The core function of a microstrip calculator is to solve the complex electromagnetic field equations governing microstrip transmission lines. While exact solutions are often intractable, several well-established approximate formulas provide high accuracy for practical engineering purposes. A common approach relies on Wheeler's incremental inductance rule or similar empirical models.

Key Formulas and Variables

The calculation typically involves determining the effective dielectric constant (εeff) first, which represents the average dielectric environment experienced by the electromagnetic wave. This value is then used to calculate the characteristic impedance (Z0) and guided wavelength (λg).

Effective Dielectric Constant (εeff)

This parameter bridges the gap between the physical dimensions and the electromagnetic wave propagation. It's a weighted average of the dielectric constant of the substrate (εr) and the surrounding air (εair ≈ 1).

For w/h > 1: $$ \epsilon_{eff} \approx \frac{\epsilon_r + 1}{2} + \frac{\epsilon_r – 1}{2} \left( 1 + 12 \frac{h}{w} \right)^{-0.5} $$

For w/h < 1: $$ \epsilon_{eff} \approx \frac{\epsilon_r + 1}{2} + \frac{\epsilon_r – 1}{2} \left( 1 + 12 \frac{h}{w} \right)^{-0.5} $$ (Note: The formula is often presented the same for both cases, but its accuracy varies. More complex formulas exist for higher precision.)

Characteristic Impedance (Z0)

This is perhaps the most critical parameter, defining the impedance matching requirements for connected components.

For w/h > 1: $$ Z_0 \approx \frac{120 \pi}{\sqrt{\epsilon_{eff}}} \left( \frac{w}{h} + 1.393 + 0.667 \ln \left( \frac{h}{w} + 1.444 \right) \right)^{-1} $$

For w/h < 1: $$ Z_0 \approx \frac{60}{\sqrt{\epsilon_{eff}}} \ln \left( \frac{8h}{w} + \frac{w}{4h} \right) $$

*Note: Trace thickness (t) is often neglected in these basic formulas for simplicity, but more advanced models incorporate it, especially for thicker traces or lower impedances.*

Guided Wavelength (λg)

This is the wavelength of the signal as it propagates along the microstrip line, influenced by the effective dielectric constant.

First, calculate the free-space wavelength (λ0): $$ \lambda_0 = \frac{c}{f} $$ where $c$ is the speed of light ($ \approx 3 \times 10^8 $ m/s) and $f$ is the frequency.

Then, calculate the guided wavelength: $$ \lambda_g = \frac{\lambda_0}{\sqrt{\epsilon_{eff}}} $$

Variables Table

Variable Meaning Unit Typical Range
h Substrate Height mm 0.1 – 5.0
w Trace Width mm 0.1 – 10.0
t Trace Thickness mm 0.018 – 0.070 (e.g., 1/2 oz, 1 oz copper)
εr Relative Dielectric Constant 2.0 (PTFE) – 15.0 (High-k ceramics)
f Frequency GHz 0.1 – 100+
Z0 Characteristic Impedance Ω 25 – 150 (Commonly 50 Ω)
εeff Effective Dielectric Constant 1.0 – εr
λg Guided Wavelength mm Varies with frequency

Practical Examples (Real-World Use Cases)

Let's explore how the microstrip calculator is used in practical PCB design scenarios.

Example 1: Designing a 50 Ohm Microstrip Line

An engineer is designing a RF power amplifier on a standard FR4 substrate (εr = 4.4) with a thickness of 1.6 mm. They need to route a signal at 2 GHz and require a 50 Ohm characteristic impedance. The trace thickness is 0.035 mm.

Inputs:

  • Substrate Height (h): 1.6 mm
  • Dielectric Constant (εr): 4.4
  • Frequency (f): 2.0 GHz
  • Trace Thickness (t): 0.035 mm
  • Target Impedance (Z0): 50 Ω

The engineer uses the microstrip calculator. They input h=1.6, εr=4.4, and f=2.0. The calculator iteratively adjusts the trace width (w) until the calculated Z0 is approximately 50 Ω. Let's assume the calculator finds that a trace width of approximately 3.0 mm is needed.

Outputs:

  • Trace Width (w): ~3.0 mm
  • Effective Dielectric Constant (εeff): ~3.15
  • Guided Wavelength (λg): ~42.5 mm

Financial Interpretation: This result tells the designer the exact physical dimension (trace width) required on the PCB layout to achieve the desired 50 Ohm impedance. This prevents signal reflections and power loss, ensuring the amplifier performs efficiently. The guided wavelength is important for designing matching networks or resonant structures.

Example 2: Calculating Wavelength for a Filter Design

A microwave engineer is designing a bandpass filter on a Rogers RO4350B substrate (εr = 3.66) with a height of 0.762 mm. The filter operates at 10 GHz. They need to know the guided wavelength to determine the physical length of filter elements. The trace width is set to 1.0 mm, and thickness is 0.035 mm.

Inputs:

  • Substrate Height (h): 0.762 mm
  • Trace Width (w): 1.0 mm
  • Trace Thickness (t): 0.035 mm
  • Dielectric Constant (εr): 3.66
  • Frequency (f): 10.0 GHz

The engineer inputs these values into the microstrip calculator.

Outputs:

  • Characteristic Impedance (Z0): ~60.5 Ω
  • Effective Dielectric Constant (εeff): ~2.78
  • Guided Wavelength (λg): ~18.1 mm

Financial Interpretation: The calculated guided wavelength of 18.1 mm is crucial. For instance, a quarter-wavelength transmission line section would be approximately 4.5 mm long. This precise length information is vital for creating filter structures like stubs or coupled lines, directly impacting the filter's performance and bandwidth. The calculated impedance of 60.5 Ω also informs the engineer about potential mismatches if connected to standard 50 Ohm systems.

How to Use This Microstrip Calculator

Using this microstrip calculator is straightforward. Follow these steps to get accurate results for your PCB designs:

  1. Gather Your Parameters: Before using the calculator, identify the key physical and material properties of your microstrip line:
    • Substrate Height (h): The thickness of the dielectric material between the ground plane and the signal trace.
    • Trace Width (w): The width of the conductive trace carrying the signal.
    • Trace Thickness (t): The thickness of the copper trace.
    • Dielectric Constant (εr): The relative permittivity of the substrate material (e.g., FR4, Rogers, Teflon).
    • Frequency (f): The operating frequency of the signal in GHz.
  2. Input the Values: Enter the gathered values into the corresponding input fields on the calculator. Ensure you use the correct units (typically mm for dimensions and GHz for frequency).
  3. Perform Calculation: Click the "Calculate" button. The calculator will process the inputs using established microstrip formulas.
  4. Review the Results: The calculator will display:
    • Primary Result: The characteristic impedance (Z0) in Ohms (Ω), prominently displayed.
    • Intermediate Values: Effective dielectric constant (εeff), guided wavelength (λg), and the trace width to height ratio (w/h).
    • Input Echo: The values you entered for trace width and substrate height are also shown for confirmation.
    • Summary Table: A complete table summarizing all input parameters and calculated results.
    • Chart: A visual representation, typically showing impedance variation against the w/h ratio.
  5. Understand the Formulas: Read the "Formula Used" section to understand the underlying approximations and principles. This helps in interpreting the results and their limitations.
  6. Use the Buttons:
    • Reset: Click "Reset" to clear all fields and return them to default values, useful for starting a new calculation.
    • Copy Results: Click "Copy Results" to copy the main result, intermediate values, and key assumptions to your clipboard for use in reports or other documents.

How to Read Results and Make Decisions

The primary output, Characteristic Impedance (Z0), is critical. For most RF systems, 50 Ohms is the standard. If your calculated Z0 deviates significantly from your target (e.g., 50 Ω), you'll need to adjust the trace width (w) or substrate height (h) and recalculate. The Effective Dielectric Constant (εeff) influences how signals propagate, affecting timing and wavelength. The Guided Wavelength (λg) is essential for designing physical structures like transmission line stubs, filters, and matching networks, where lengths are often specified as fractions of a wavelength.

Key Factors That Affect Microstrip Results

Several factors influence the accuracy and behavior of microstrip lines, impacting the results from any microstrip calculator:

  1. Substrate Height (h): A larger substrate height generally leads to a lower characteristic impedance for a given trace width. It also affects the effective dielectric constant and wavelength. Precise control over 'h' is crucial for impedance matching.
  2. Trace Width (w): This is the primary geometric parameter used to control impedance. A wider trace (relative to 'h') results in lower impedance, while a narrower trace increases impedance. The relationship is non-linear.
  3. Dielectric Constant (εr): A higher εr concentrates the electromagnetic fields more within the substrate, leading to a higher effective dielectric constant (εeff). This, in turn, results in a lower guided wavelength (λg) and typically a lower characteristic impedance (Z0) for a given geometry. Material consistency is key.
  4. Trace Thickness (t): While often ignored in basic calculators, trace thickness significantly impacts impedance, especially for lower impedance lines (wider traces). Thicker copper reduces conductor losses and lowers the effective impedance. Advanced calculators account for this.
  5. Frequency (f): While the quasi-static formulas used in many calculators assume frequency independence for impedance, wavelength is directly dependent on frequency. More importantly, at higher frequencies, conductor losses (skin effect) and dielectric losses become significant, deviating from the ideal lossless model. Dispersion effects also alter εeff and Z0 slightly.
  6. Manufacturing Tolerances: Variations in substrate height (h), trace width (w), and dielectric constant (εr) during PCB manufacturing are unavoidable. These tolerances directly affect the actual impedance achieved, potentially causing signal integrity issues if not accounted for. Understanding the PCB fabricator's capabilities is essential.
  7. Edge Effects and Surface Roughness: The formulas are approximations. Real-world effects like the exact shape of the trace edges and the roughness of the copper surface (especially at high frequencies due to skin effect) can subtly alter the electromagnetic field distribution and thus the impedance and losses.

Frequently Asked Questions (FAQ)

Q1: What is the most common microstrip impedance? A1: The most common characteristic impedance for microstrip lines in RF and microwave systems is 50 Ohms (Ω). 75 Ohms is also frequently used, particularly in video and some communication systems.
Q2: Does trace thickness affect impedance? A2: Yes, especially for lower impedance values (e.g., below 40 Ω) or when the trace thickness is a significant fraction of the substrate height. Thicker traces generally lead to lower impedance. Basic calculators might ignore this for simplicity.
Q3: Why is the effective dielectric constant (εeff) different from the substrate's dielectric constant (εr)? A3: The electromagnetic wave in a microstrip line propagates through both the dielectric substrate (with εr) and the air above it (with ε ≈ 1). The εeff is a weighted average representing the overall dielectric environment the wave experiences, and it's always between 1 and εr.
Q4: How accurate are the formulas used in this microstrip calculator? A4: The formulas (like Wheeler's or Hammerstad's) are highly accurate approximations for typical microstrip dimensions and materials, often within 1-2% for impedance. However, accuracy can decrease for very small or very large w/h ratios, very thin substrates, or extremely high frequencies where losses and dispersion become dominant.
Q5: Can I use this calculator for stripline? A5: No, this calculator is specifically for microstrip, which has a single trace above a ground plane separated by dielectric. Stripline has a trace embedded between two ground planes. The formulas for stripline are different.
Q6: What happens if my trace width is much larger than the substrate height? A6: When w/h is large, the fields spread out more into the air, making the effective dielectric constant (εeff) closer to 1. This results in a lower characteristic impedance (Z0) and a guided wavelength (λg) closer to the free-space wavelength (λ0).
Q7: How do I achieve a specific impedance, like 50 Ohms? A7: You typically adjust the trace width (w) while keeping the substrate height (h) and dielectric constant (εr) fixed. Use the calculator to find the 'w' that yields the desired Z0. You might need to iterate or use a more advanced calculator/simulator if trace thickness is also a factor.
Q8: Are conductor losses considered? A8: Basic quasi-static formulas used in many simple calculators do not explicitly include conductor losses (due to skin effect) or dielectric losses. These losses become more significant at higher frequencies and can slightly alter the effective impedance and introduce signal attenuation. For precise high-frequency design, electromagnetic simulators are recommended.

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var speedOfLight = 299792458; // meters per second function validateInput(id, min, max, name) { var input = document.getElementById(id); var errorElement = document.getElementById(id + "Error"); var value = parseFloat(input.value); errorElement.style.display = 'none'; // Hide error by default if (isNaN(value)) { errorElement.textContent = name + " is required."; errorElement.style.display = 'block'; return false; } if (value <= 0) { errorElement.textContent = name + " must be positive."; errorElement.style.display = 'block'; return false; } if (min !== null && value max) { errorElement.textContent = name + " must be no more than " + max + "."; errorElement.style.display = 'block'; return false; } return true; } function calculateMicrostrip() { // Clear previous errors var errorElements = document.querySelectorAll('.error-message'); for (var i = 0; i 1 and w/h 1) { var term_z0 = (w / h) + 1.393 + 0.667 * Math.log(h / w + 1.444); Z0 = (120 * Math.PI / Math.sqrt(epsilon_eff)) / term_z0; } else { var term_z0 = (8 * h / w) + (w / (4 * h)); Z0 = (60 / Math.sqrt(epsilon_eff)) * Math.log(term_z0); } // Adjust Z0 slightly for trace thickness (simplified empirical correction) // This is a very basic adjustment; real models are more complex. if (t / h < 0.1) { // Only apply if trace is relatively thin compared to height var t_correction = 1 – (t / h); // Simple linear reduction factor Z0 = Z0 * t_correction; } // Calculate Guided Wavelength (lambda_g) var c_mps = speedOfLight; // m/s var f_hz = f_ghz * 1e9; // Hz var lambda_0_m = c_mps / f_hz; // Free space wavelength in meters var lambda_0_mm = lambda_0_m * 1000; // Free space wavelength in mm lambda_g_mm = lambda_0_mm / Math.sqrt(epsilon_eff); // Update Results Display document.getElementById("impedanceResult").textContent = Z0.toFixed(2); document.getElementById("effResult").textContent = epsilon_eff.toFixed(3); document.getElementById("lambdaGResult").textContent = lambda_g_mm.toFixed(2); document.getElementById("whRatioResult").textContent = wh_ratio.toFixed(2); document.getElementById("traceWidthResult").textContent = w.toFixed(3); document.getElementById("substrateHeightResult").textContent = h.toFixed(3); // Update Table document.getElementById("tableZ0").textContent = Z0.toFixed(2); document.getElementById("tableEff").textContent = epsilon_eff.toFixed(3); document.getElementById("tableLambdaG").textContent = lambda_g_mm.toFixed(2); document.getElementById("tableWhRatio").textContent = wh_ratio.toFixed(2); document.getElementById("tableSubstrateHeight").textContent = h.toFixed(3); document.getElementById("tableTraceWidth").textContent = w.toFixed(3); document.getElementById("tableTraceThickness").textContent = t.toFixed(4); document.getElementById("tableDielectricConstant").textContent = epsilon_r.toFixed(2); document.getElementById("tableFrequency").textContent = f_ghz.toFixed(2); updateChart(); } function resetCalculator() { document.getElementById("substrateHeight").value = "1.6"; document.getElementById("traceWidth").value = "2.0"; document.getElementById("traceThickness").value = "0.035"; document.getElementById("dielectricConstant").value = "4.4"; document.getElementById("frequency").value = "1.0"; // Clear results and errors document.getElementById("impedanceResult").textContent = "–"; document.getElementById("effResult").textContent = "–"; document.getElementById("lambdaGResult").textContent = "–"; document.getElementById("whRatioResult").textContent = "–"; document.getElementById("traceWidthResult").textContent = "–"; document.getElementById("substrateHeightResult").textContent = "–"; var tableCells = document.querySelectorAll("#resultsTableBody td"); for (var i = 0; i < tableCells.length; i++) { tableCells[i].textContent = "–"; } var errorElements = document.querySelectorAll('.error-message'); for (var i = 0; i < errorElements.length; i++) { errorElements[i].style.display = 'none'; } // Clear chart var canvas = document.getElementById('impedanceChart'); var ctx = canvas.getContext('2d'); ctx.clearRect(0, 0, canvas.width, canvas.height); } function copyResults() { var impedance = document.getElementById("impedanceResult").textContent; var eff = document.getElementById("effResult").textContent; var lambdaG = document.getElementById("lambdaGResult").textContent; var whRatio = document.getElementById("whRatioResult").textContent; var traceW = document.getElementById("traceWidthResult").textContent; var subH = document.getElementById("substrateHeightResult").textContent; var assumptions = "Key Assumptions:\n"; assumptions += "- Substrate Height (h): " + document.getElementById("substrateHeight").value + " mm\n"; assumptions += "- Trace Width (w): " + document.getElementById("traceWidth").value + " mm\n"; assumptions += "- Trace Thickness (t): " + document.getElementById("traceThickness").value + " mm\n"; assumptions += "- Dielectric Constant (εr): " + document.getElementById("dielectricConstant").value + "\n"; assumptions += "- Frequency (f): " + document.getElementById("frequency").value + " GHz\n"; var resultsText = "Microstrip Calculation Results:\n\n"; resultsText += "Characteristic Impedance (Z0): " + impedance + " Ω\n"; resultsText += "Effective Dielectric Constant (εeff): " + eff + "\n"; resultsText += "Guided Wavelength (λg): " + lambdaG + " mm\n"; resultsText += "Trace Width/Height Ratio (w/h): " + whRatio + "\n"; resultsText += "Trace Width (w): " + traceW + " mm\n"; resultsText += "Substrate Height (h): " + subH + " mm\n\n"; resultsText += assumptions; // Use navigator.clipboard for modern browsers if (navigator.clipboard && navigator.clipboard.writeText) { navigator.clipboard.writeText(resultsText).then(function() { alert("Results copied to clipboard!"); }).catch(function(err) { console.error("Failed to copy text: ", err); fallbackCopyTextToClipboard(resultsText); }); } else { fallbackCopyTextToClipboard(resultsText); } } // Fallback for older browsers function fallbackCopyTextToClipboard(text) { var textArea = document.createElement("textarea"); textArea.value = text; textArea.style.position = "fixed"; // Avoid scrolling to bottom textArea.style.left = "-9999px"; textArea.style.top = "-9999px"; document.body.appendChild(textArea); textArea.focus(); textArea.select(); try { var successful = document.execCommand('copy'); var msg = successful ? 'successful' : 'unsuccessful'; alert('Results ' + msg + ' copied to clipboard!'); } catch (err) { console.error('Fallback: Oops, unable to copy', err); alert('Failed to copy results. Please copy manually.'); } document.body.removeChild(textArea); } function updateChart() { var canvas = document.getElementById('impedanceChart'); var ctx = canvas.getContext('2d'); ctx.clearRect(0, 0, canvas.width, canvas.height); // Clear previous drawing var h = parseFloat(document.getElementById("substrateHeight").value); var epsilon_r = parseFloat(document.getElementById("dielectricConstant").value); var max_wh_ratio = 5.0; // Max w/h ratio to plot var num_points = 50; var dataPoints = []; // Generate data points for the chart for (var i = 0; i < num_points; i++) { var wh_ratio = (i / (num_points – 1)) * max_wh_ratio; if (wh_ratio 1) { var term_z0 = (current_w / h) + 1.393 + 0.667 * Math.log(h / current_w + 1.444); current_Z0 = (120 * Math.PI / Math.sqrt(current_epsilon_eff)) / term_z0; } else { var term_z0 = (8 * h / current_w) + (current_w / (4 * h)); current_Z0 = (60 / Math.sqrt(current_epsilon_eff)) * Math.log(term_z0); } // Basic thickness correction (optional, can make chart less clean if t varies) // var t = parseFloat(document.getElementById("traceThickness").value); // if (t / h < 0.1) { // current_Z0 = current_Z0 * (1 – (t / h)); // } dataPoints.push({ wh: wh_ratio, z0: current_Z0 }); } // Chart dimensions and margins var chartWidth = canvas.clientWidth; var chartHeight = canvas.clientHeight; var margin = { top: 20, right: 20, bottom: 50, left: 60 }; var plotWidth = chartWidth – margin.left – margin.right; var plotHeight = chartHeight – margin.top – margin.bottom; // Find min/max Z0 for scaling var minZ0 = 25; // Typical minimum var maxZ0 = 150; // Typical maximum dataPoints.forEach(function(point) { if (point.z0 maxZ0) maxZ0 = point.z0; }); maxZ0 = Math.ceil(maxZ0 / 10) * 10; // Round up to nearest 10 // Scales var xScale = function(wh) { return margin.left + (wh / max_wh_ratio) * plotWidth; }; var yScale = function(z0) { return chartHeight – margin.bottom – ((z0 – minZ0) / (maxZ0 – minZ0)) * plotHeight; }; // Draw Axes ctx.beginPath(); ctx.moveTo(margin.left, margin.top); ctx.lineTo(margin.left, chartHeight – margin.bottom); // Y-axis ctx.lineTo(chartWidth – margin.right, chartHeight – margin.bottom); // X-axis ctx.strokeStyle = '#ccc'; ctx.lineWidth = 1; ctx.stroke(); // X-axis Labels (w/h ratio) ctx.fillStyle = '#333′; ctx.font = '12px Segoe UI'; ctx.textAlign = 'center'; ctx.fillText('0', margin.left, chartHeight – margin.bottom + 15); ctx.fillText(max_wh_ratio.toFixed(1), chartWidth – margin.right, chartHeight – margin.bottom + 15); ctx.fillText('w/h Ratio', chartWidth / 2, chartHeight – 10); // Y-axis Labels (Impedance) ctx.textAlign = 'right'; ctx.textBaseline = 'middle'; var numYLabels = 5; for (var i = 0; i <= numYLabels; i++) { var yValue = minZ0 + (i / numYLabels) * (maxZ0 – minZ0); var yPos = yScale(yValue); ctx.fillText(yValue.toFixed(0) + ' Ω', margin.left – 10, yPos); } ctx.save(); ctx.translate(margin.left – 40, chartHeight / 2); ctx.rotate(-90 * Math.PI / 180); ctx.fillText('Impedance (Z0)', 0, 0); ctx.restore(); // Draw Data Series (Impedance) ctx.beginPath(); ctx.strokeStyle = 'var(–primary-color)'; ctx.lineWidth = 2; for (var i = 0; i < dataPoints.length; i++) { var x = xScale(dataPoints[i].wh); var y = yScale(dataPoints[i].z0); if (i === 0) { ctx.moveTo(x, y); } else { ctx.lineTo(x, y); } } ctx.stroke(); // Mark current input point var current_wh = parseFloat(document.getElementById("traceWidth").value) / parseFloat(document.getElementById("substrateHeight").value); var current_Z0_val = parseFloat(document.getElementById("impedanceResult").textContent); if (!isNaN(current_wh) && !isNaN(current_Z0_val) && current_wh <= max_wh_ratio) { var currentX = xScale(current_wh); var currentY = yScale(current_Z0_val); ctx.fillStyle = 'var(–success-color)'; ctx.beginPath(); ctx.arc(currentX, currentY, 5, 0, 2 * Math.PI); // Draw a circle ctx.fill(); } } // Initial calculation and chart draw on load window.onload = function() { calculateMicrostrip(); updateChart(); // Initial chart draw document.getElementById('currentYear').textContent = new Date().getFullYear(); }; // Update results and chart in real-time as inputs change var inputFields = document.querySelectorAll('#calculator-form input[type="number"], #calculator-form select'); for (var i = 0; i < inputFields.length; i++) { inputFields[i].addEventListener('input', function() { calculateMicrostrip(); updateChart(); }); }

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