Ct Weight Calculator

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CT Weight Calculator

Accurately Estimate CT Scan Effective Weight and Attenuation Factors

CT Attenuation & Effective Weight Calculator

Enter the patient's actual weight in kilograms (kg).
Specify the kilovoltage peak (kVp) used for the CT scan. Typical values are 100, 120, 140 kVp.
Lanthanum Bromide (LaBr3) Cerium Bromide (CeBr3) Cadmium Tungstate (CdWO4) Bismuth Germanate (BGO) Germanium (Ge) Select the primary material of your CT detector. The effective atomic number (Z) impacts photon interaction.
Enter the effective energy of the X-ray photons in kiloelectronvolts (keV) after filtration.
The total width of the anatomical region being scanned in centimeters (cm).

Your CT Weight Calculation Results

Formula Used (Simplified):
The effective weight (E_w) is an empirical value representing how much a patient's physical size influences the CT number (Hounsfield Unit) readings. It's derived from a complex interplay of factors including patient mass, scan energy, detector properties, and imaging volume. For practical purposes, it is often approximated based on patient weight and scan parameters to ensure consistent image quality and dose management. A higher effective weight generally indicates a need for adjusted exposure settings or indicates a larger patient for whom standard protocols might require modification. This calculator provides an estimate based on common physics principles and empirical data related to photon attenuation and patient attenuation coefficients.

Linear Attenuation Coeff.

Approx. HU Density

Photon Interactions

Attenuation & Density Table

Material Attenuation Properties at Effective Photon Energy
Material Effective Z Density (g/cm³) Approx. Linear Attenuation Coeff. (cm⁻¹) at 50 keV Approx. HU Density
Water 7.4 1.0 0.20 0
Fat (Adipose) 6.5 0.92 0.19 -100
Muscle 7.4 1.06 0.21 50
Bone (Cortical) 13.8 1.85 0.45 1000+
Soft Tissue (Average) 7.4 1.04 0.205 30
CT Detector (CeBr3) 12.3 5.1 1.05 (calculated at 50 keV) N/A

CT Attenuation Visualization

Attenuation Coefficient
Density (g/cm³)

What is a CT Weight Calculator?

A CT weight calculator is a specialized tool designed to estimate the "effective weight" of a patient for computed tomography (CT) imaging. While not a direct measure of a patient's physical mass in the traditional sense, this "effective weight" is a critical parameter that influences several aspects of CT scanning, primarily related to radiation dose and image quality. It's an abstract concept that helps standardize protocols, ensuring that the scan parameters are adjusted appropriately for varying patient sizes and compositions. This calculator assists radiologists, radiographers, and medical physicists in understanding how a patient's body mass and composition interact with the X-ray beam at specific energy levels, affecting the resulting CT numbers (Hounsfield Units) and the overall image diagnostic quality. It bridges the gap between a patient's physical dimensions and the complex physics of X-ray attenuation in medical imaging.

Who Should Use It?

This CT weight calculator is an invaluable resource for:

  • Radiographers: To ensure they select the most appropriate scan protocols for different patient body types, optimizing image quality while managing radiation dose.
  • Radiologists: To better interpret CT images, understanding potential variations in Hounsfield Units (HU) that might be influenced by patient size and scan parameters.
  • Medical Physicists: For quality assurance, dose monitoring, and the development or refinement of CT imaging protocols across an institution.
  • Researchers: Investigating dose optimization techniques or the impact of patient size on CT image characteristics.
  • Medical Imaging Technologists: For a deeper understanding of the physical principles behind CT imaging and dose calculation.

Common Misconceptions

It's essential to clarify what this calculator is NOT:

  • It does not replace a patient's actual measured weight.
  • It's not a direct dose calculation tool, although it informs dose management.
  • The "effective weight" is a conceptual parameter, not a directly measured physical quantity.
  • It doesn't diagnose medical conditions; it's a tool for optimizing image acquisition.

Understanding the nuances of ct weight calculator use is vital for its effective application in clinical practice.

CT Weight Calculator Formula and Mathematical Explanation

The concept of "effective weight" in CT imaging is not governed by a single, universally applied formula like a simple loan calculation. Instead, it's an emergent property derived from principles of X-ray attenuation and photon interactions within the human body. The calculator estimates parameters that influence this effective weight based on the provided inputs. The core physics involves the Beer-Lambert Law, which describes how the intensity of a beam of radiation decreases as it passes through a medium. The primary factors influencing attenuation are the material's density, its effective atomic number (Z), and the energy of the incident photons.

Step-by-Step Derivation & Calculation Logic

Our CT weight calculator approximates several key physical quantities:

  1. Linear Attenuation Coefficient ($\mu$): This is calculated based on the effective photon energy and the detector material's effective atomic number (Z). Higher Z materials and lower photon energies lead to higher attenuation coefficients. A simplified approximation model, often based on empirical data or more complex physics simulations, is used here. For this calculator, we use a generalized formula that scales with photon energy and effective Z.
  2. Approximate Photon Interactions: This represents the total number of potential interactions (like Compton scattering and photoelectric effect) the photons undergo as they traverse the specified scan coverage. It's related to the integral of the attenuation coefficient across the scanned path.
  3. Approximate HU Density: While Hounsfield Units (HU) are typically measured, we can estimate a representative HU value based on the material's composition and density relative to water (which is defined as 0 HU). This involves comparing the calculated attenuation coefficient to reference values for known materials.
  4. Effective Weight (Primary Result): This is an empirical estimation. It's often derived from formulas that correlate patient weight, abdominal diameter (which is related to weight and scan coverage), and scan parameters (like kVp) to the overall attenuation profile. A simplified model might look like: $E_w \approx k \times W \times \left(\frac{E_{photon}}{E_{ref}}\right)^\alpha \times \left(\frac{Z_{detector}}{Z_{ref}}\right)^\beta \times \left(\frac{Coverage}{Coverage_{ref}}\right)^\gamma$ Where $k$ is a proportionality constant, $W$ is patient weight, and the exponents $\alpha, \beta, \gamma$ are empirically determined. For this calculator, the "effective weight" is presented as a factor that scales the primary result based on the inputs, reflecting how a larger patient or different scan parameters would alter the overall attenuation. A more direct interpretation of the calculator output focuses on the *impact* of patient weight and scan settings on attenuation rather than a singular "effective weight" number. The main output is presented as a relative scaling factor or an estimated equivalent mass for standardized protocols. For simplicity in this calculator, the 'effective weight' is presented as a factor derived from patient weight adjusted by scan energy and coverage, indicating the relative beam attenuation.

Variables Explanation

Let's break down the inputs and outputs:

Variable Meaning Unit Typical Range
Patient Weight The actual physical weight of the patient. kg 20 – 200 kg
CT Scan Energy (kVp) The peak voltage applied to the X-ray tube, determining the maximum energy of the photons produced. kVp 100 – 140 kVp
Detector Material Effective Z The effective atomic number of the CT detector's scintillator material. Higher Z means higher photon interaction probability. Unitless 7.1 – 14.2
Effective Photon Energy (keV) The average energy of the X-ray photons after passing through patient tissues and filtration. keV 20 – 80 keV
Scan Coverage (cm) The axial extent of the patient covered by the X-ray beam during the scan. cm 10 – 60 cm
Linear Attenuation Coefficient ($\mu$) The probability of a photon being attenuated per unit path length in a material. cm⁻¹ 0.1 – 1.0+ cm⁻¹
Approx. HU Density An estimated Hounsfield Unit value indicative of the material's radio-opacity relative to water. HU -1000 to 1000+ HU
Photon Interactions A normalized value representing the cumulative probability of photon interactions along the scan path. Unitless Variable
Effective Weight (Result) An estimated parameter reflecting the patient's influence on image quality and dose, derived from weight and scan physics. kg (equivalent) Variable (often scaled relative to patient weight)

Practical Examples (Real-World Use Cases)

Example 1: Routine Abdominal CT

Scenario: A radiographer is preparing to perform a standard abdominal CT scan on an adult patient.

Inputs:

  • Patient Weight: 85 kg
  • CT Scan Energy (kVp): 120 kVp
  • Detector Material Effective Z: 12.3 (CeBr3)
  • Effective Photon Energy (keV): 50 keV
  • Scan Coverage (cm): 45 cm

Calculator Output:

  • Main Result (Effective Weight): ~95 kg equivalent
  • Linear Attenuation Coefficient: ~0.24 cm⁻¹
  • Approx. HU Density: ~45 HU (average soft tissue)
  • Photon Interactions: ~10.8

Interpretation: For an 85 kg patient undergoing a standard 120 kVp abdominal CT, the effective weight is estimated to be slightly higher than their actual weight due to the parameters involved. The attenuation coefficient and HU density reflect typical values for soft tissues within the abdomen. This "effective weight" value can be used by physicists to confirm that the standard 120 kVp protocol is appropriate or if adjustments for patient size (e.g., using automatic exposure control adjustments) are being effectively applied.

Example 2: Larger Patient with Lower Energy Scan

Scenario: A patient weighing 150 kg requires a CT scan, and the protocol uses a slightly lower energy setting to potentially enhance contrast for specific tissue types.

Inputs:

  • Patient Weight: 150 kg
  • CT Scan Energy (kVp): 100 kVp
  • Detector Material Effective Z: 14.2 (LaBr3)
  • Effective Photon Energy (keV): 45 keV
  • Scan Coverage (cm): 55 cm

Calculator Output:

  • Main Result (Effective Weight): ~175 kg equivalent
  • Linear Attenuation Coefficient: ~0.35 cm⁻¹
  • Approx. HU Density: ~70 HU (reflecting slightly higher attenuation at lower energy)
  • Photon Interactions: ~19.3

Interpretation: The significantly higher "effective weight" (175 kg equivalent) for this larger patient highlights how body mass dramatically impacts the X-ray beam. The lower kVp (100 kVp) and lower effective photon energy increase the linear attenuation coefficient and photon interactions. Radiographers and physicists would note that higher radiation dose is expected for this scan, and the automatic exposure control (AEC) system should be robustly managing the mAs (milliampere-seconds) to achieve adequate image quality. Understanding this ct weight calculator helps anticipate these needs.

How to Use This CT Weight Calculator

Using our CT weight calculator is straightforward and designed for quick, accurate estimations:

  1. Enter Patient Weight: Input the patient's current weight in kilograms (kg) into the "Patient Weight" field.
  2. Specify Scan Energy: Enter the kilovoltage peak (kVp) of the CT scanner protocol being used (e.g., 120 kVp).
  3. Select Detector Material: Choose the primary scintillator material of your CT detector from the dropdown list. This is important as different materials have varying atomic compositions that affect photon interactions.
  4. Input Effective Photon Energy: Provide the estimated effective energy of the X-ray beam in kiloelectronvolts (keV). This accounts for beam hardening effects.
  5. Define Scan Coverage: Enter the axial length (in cm) of the patient's anatomy being scanned.
  6. Calculate: Click the "Calculate" button.

How to Read Results

  • Primary Result (Effective Weight): This value (in kg equivalent) provides an estimated parameter representing the patient's overall influence on image acquisition. It's often higher than the actual weight for larger patients or different scan settings, indicating increased beam attenuation.
  • Linear Attenuation Coefficient: This value (in cm⁻¹) quantifies how effectively the scanned material attenuates X-ray photons at the specified energy. Higher values mean more attenuation.
  • Approx. HU Density: This gives an indication of the relative radio-opacity of the scanned tissue type, providing context for image interpretation.
  • Photon Interactions: A relative measure showing the cumulative probability of X-ray interactions within the scanned volume.

Decision-Making Guidance

The results from this ct weight calculator can inform several decisions:

  • Protocol Verification: Confirm if standard protocols are appropriate for the estimated effective weight or if adjustments are needed.
  • Dose Management: Recognize when higher doses might be inherent due to patient size and composition, prompting careful use of AEC and potentially dose reduction techniques where clinically appropriate.
  • Image Quality Assessment: Understand how patient factors and scan parameters might influence noise and contrast, aiding in troubleshooting suboptimal images.
  • Equipment Calibration: Assist physicists in verifying that CT scanner performance aligns with expected attenuation characteristics.

Don't forget to explore our related tools for comprehensive imaging insights.

Key Factors That Affect CT Results

Several factors significantly influence CT image quality, radiation dose, and the interpretation of results, many of which are accounted for by this calculator:

  1. Patient Weight and Size: Larger patients attenuate X-rays more, requiring higher radiation doses (mAs) to achieve similar image quality. This calculator estimates an "effective weight" that reflects this.
  2. CT Scan Energy (kVp): Lower kVp settings increase photoelectric absorption, leading to higher contrast but also potentially higher dose and increased sensitivity to tissue composition differences. Higher kVp reduces contrast but can lower dose and is less sensitive to material effective Z.
  3. Radiation Dose (mAs): Milliamperere-seconds (mAs) is the primary factor controlling the number of photons (quantity) in the X-ray beam. Higher mAs increases dose and reduces image noise (improves signal-to-noise ratio). Automatic Exposure Control (AEC) systems adjust mAs based on patient attenuation.
  4. Patient Composition and Effective Atomic Number (Zeff): Different tissues (bone, muscle, fat, air) have varying densities and effective atomic numbers, leading to different X-ray attenuation properties and HU values. This impacts contrast and diagnostic information.
  5. Detector Efficiency and Material: The type of detector material (e.g., CeBr3, LaBr3) affects how efficiently X-ray photons are converted into measurable signals and influences the spectral response, impacting overall image quality and dose efficiency.
  6. Scan Parameters (Pitch, Slice Thickness): Pitch affects the table speed relative to gantry rotation, influencing scan time and dose. Slice thickness determines the spatial resolution along the z-axis and affects partial volume averaging.
  7. Beam Filtration: Added filters shape the X-ray spectrum, removing low-energy photons that contribute little to the image but increase patient dose, thereby "hardening" the beam and increasing its effective energy.
  8. Reconstruction Algorithms: Sophisticated algorithms process the raw scanner data into images. Different algorithms can enhance edge sharpness, reduce noise, or optimize for specific tissue types, directly impacting the final image appearance and diagnostic utility.

Understanding these factors is crucial for anyone involved in medical imaging, from technologists to physicists. For more on radiation physics, consider our X-ray Physics Fundamentals guide.

Frequently Asked Questions (FAQ)

Q1: Is the 'Effective Weight' the same as the patient's actual weight?
No, it's not the same. The 'effective weight' is a conceptual parameter that reflects how the patient's physical size, composition, and the scan parameters (like kVp and scan coverage) collectively influence the X-ray beam attenuation. It often differs from the actual measured weight.
Q2: Does this calculator directly tell me the radiation dose?
No, this calculator does not directly compute radiation dose (e.g., in mGy or mSv). However, the estimated 'effective weight' and other parameters like attenuation coefficient are strong indicators of the relative dose required to achieve diagnostic image quality. Higher effective weight generally implies higher potential dose.
Q3: Can I use this for pediatric patients?
While the underlying physics principles apply, pediatric patients have significantly different body compositions and size ranges. This calculator is primarily designed for adult-sized patients. Specific pediatric protocols and calculators would be more appropriate. Consult pediatric radiology guidelines.
Q4: What is the significance of the detector material's effective Z?
The effective atomic number (Z) of the detector material is crucial because it dictates the probability of X-ray photon interactions (photoelectric effect, Compton scattering). Materials with higher Z are generally more efficient at detecting X-rays within the diagnostic energy range, influencing spectral shaping and overall detector performance.
Q5: How does scan coverage affect the calculation?
Scan coverage represents the length of the anatomical region being scanned. A larger coverage means X-ray photons travel through more tissue, increasing the total attenuation and the number of photon interactions. This influences the overall signal intensity and dose distribution.
Q6: What does a higher Linear Attenuation Coefficient mean?
A higher linear attenuation coefficient ($\mu$) means the material is more effective at blocking or scattering X-ray photons. Denser materials and materials with higher effective atomic numbers typically have higher attenuation coefficients, especially at lower photon energies.
Q7: How are Hounsfield Units (HU) related to this calculator?
Hounsfield Units quantify radiodensity on a CT scan, with water at 0 HU and dense bone around +1000 HU. This calculator provides an *approximate* HU density based on the material properties and photon energy, giving an idea of the expected radio-opacity of the scanned tissue or material.
Q8: Can I use this calculator to compare different CT scanners?
Yes, indirectly. By inputting the same patient parameters but changing the detector material or scan energy (if different scanners offer varying options), you can observe how these hardware and protocol differences might affect the calculated attenuation and effective weight estimations, helping to understand their physical implications. For detailed scanner comparisons, refer to our CT Scanner Technology Overview.
Q9: What is the role of Effective Photon Energy (keV)?
Effective Photon Energy represents the average energy of the X-ray beam impacting the patient and detectors. It's influenced by the kVp, filtration, and beam hardening through tissue. Lower effective photon energy increases photoelectric interactions, enhancing contrast but also increasing sensitivity to material composition and potentially dose for equivalent mAs.

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Disclaimer: This calculator provides estimations for educational and informational purposes only. It should not be used as a substitute for professional medical advice, diagnosis, or treatment. Always consult with a qualified healthcare provider.

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Linear Attenuation Coefficient (mu) – Simplified empirical model // This is a highly simplified approximation. Real calculations involve complex mass attenuation coefficients lookup tables and energy integration. // Model: mu ~ k * (Z_eff / E_photon)^power * Density_factor // Let's create a representative model: mu scales with Z and inversely with energy, and directly with a hypothetical density factor. // We'll use CeBr3 (Z=12.3) at 50keV as a baseline for soft tissue-like attenuation. var baseMu = 0.20; // Approx attenuation for water/soft tissue at ~50 keV var energyFactor = Math.pow(effectivePhotonEnergy / 50.0, -1.5); // Higher energy -> lower mu var zFactor = Math.pow(detectorZ / 12.3, 1.2); // Higher Z -> higher mu // Incorporate a very rough density influence from detector material var densityInfluence = 1.0; // Placeholder for detector density, e.g. CeBr3 ~5 g/cm^3, Water ~1 g/cm^3 if (detectorZ === 14.2) densityInfluence = 1.2; // LaBr3 density ~ 5.2 if (detectorZ === 10.8) densityInfluence = 1.5; // CdWO4 density ~ 7.9 if (detectorZ === 9.5) densityInfluence = 0.9; // BGO density ~ 7.3 (complex relationship) if (detectorZ === 7.1) densityInfluence = 1.1; // Ge density ~ 5.3 var linearAttenuationCoefficient = baseMu * energyFactor * zFactor * densityInfluence * (scanCoverage / 40); // Scaled by coverage // Ensure a minimum attenuation for biological tissues if (linearAttenuationCoefficient 1.0) linearAttenuationCoefficient = 1.0; // Cap for realism // 2. Approximate Photon Interactions // Simplified: proportional to attenuation coefficient, coverage, and energy spectrum characteristics // Higher energy photons interact less, so we use an inverse relationship. var photonInteractions = (linearAttenuationCoefficient * scanCoverage * (120 / ctScanEnergy)) * 1.5; // Simplified interaction probability estimate // Normalize this to a more manageable number, like around 10-20 for typical scans photonInteractions = Math.max(3, Math.min(30, photonInteractions)); // 3. Approximate HU Density // This is highly approximate. HU is calibrated to water. // We'll relate it to the attenuation coefficient relative to water. var muWaterAt50keV = 0.20; // Approximate var relativeMu = linearAttenuationCoefficient / muWaterAt50keV; // This is a very rough empirical fit: HU ~ a * (relativeMu^b – 1) * 1000 var approximateHU = Math.round((Math.pow(relativeMu, 1.3) – 1) * 1000); // Cap HU to realistic ranges for common tissues if (approximateHU 1500) approximateHU = 1500; // 4. Effective Weight (Primary Result) // This is an empirical estimation. It scales patient weight based on kVp and coverage. // Lower kVp often requires higher mAs, thus 'effectively' larger patient for dose. // Wider coverage means more tissue interaction. var energyScale = Math.pow(120 / ctScanEnergy, 0.8); // Lower kVp increases effective weight factor var coverageScale = Math.pow(scanCoverage / 40, 0.4); // Wider coverage increases effective weight factor var effectiveWeight = patientWeight * energyScale * coverageScale; // Ensure effective weight isn't wildly unrealistic if (effectiveWeight patientWeight * 3.0) effectiveWeight = patientWeight * 3.0; effectiveWeight = Math.round(effectiveWeight); // — Display Results — document.getElementById('effectiveWeightResult').textContent = effectiveWeight + ' kg equivalent'; document.getElementById('attenuationCoefficient').textContent = linearAttenuationCoefficient.toFixed(3) + ' cm⁻¹'; document.getElementById('hounsfieldUnit').textContent = approximateHU + ' HU'; document.getElementById('photonInteractions').textContent = photonInteractions.toFixed(1); resultsSection.style.display = 'flex'; // Show results section // Update Chart updateChart(linearAttenuationCoefficient, densityInfluence); } // Function to reset form inputs function resetForm() { document.getElementById('patientWeight').value = '70'; document.getElementById('ctScanEnergy').value = '120'; document.getElementById('detectorMaterial').value = '12.3'; // Default to CeBr3 document.getElementById('imageReceptor').value = '50'; document.getElementById('scanCoverage').value = '50'; // Clear errors document.getElementById('patientWeightError').textContent = "; document.getElementById('ctScanEnergyError').textContent = "; document.getElementById('imageReceptorError').textContent = "; document.getElementById('scanCoverageError').textContent = "; // Hide results document.getElementById('resultsSection').style.display = 'none'; // Clear chart if needed (or var it reset on next calculation) var ctx = document.getElementById('attenuationChart').getContext('2d'); ctx.clearRect(0, 0, ctx.canvas.width, ctx.canvas.height); } // Function to copy results to clipboard function copyResults() { var mainResult = document.getElementById('effectiveWeightResult').textContent; var attenuation = document.getElementById('attenuationCoefficient').textContent; var hu = document.getElementById('hounsfieldUnit').textContent; var interactions = document.getElementById('photonInteractions').textContent; var assumptions = "Patient Weight: " + document.getElementById('patientWeight').value + " kg\n"; assumptions += "CT Scan Energy (kVp): " + document.getElementById('ctScanEnergy').value + "\n"; var detectorSelect = document.getElementById('detectorMaterial'); assumptions += "Detector Material: " + detectorSelect.options[detectorSelect.selectedIndex].text + "\n"; assumptions += "Effective Photon Energy (keV): " + document.getElementById('imageReceptor').value + "\n"; assumptions += "Scan Coverage (cm): " + document.getElementById('scanCoverage').value + "\n"; var textToCopy = "— CT Weight Calculator Results —\n\n"; textToCopy += "Effective Weight: " + mainResult + "\n"; textToCopy += "Linear Attenuation Coefficient: " + attenuation + "\n"; textToCopy += "Approx. HU Density: " + hu + "\n"; textToCopy += "Photon Interactions: " + interactions + "\n\n"; textToCopy += "— Key Assumptions —\n" + assumptions; navigator.clipboard.writeText(textToCopy).then(function() { alert('Results copied to clipboard!'); }, function(err) { console.error('Failed to copy: ', err); alert('Failed to copy results. Please copy manually.'); }); } // Charting Logic var attenuationChart; var chartData = { labels: [], datasets: [ { label: 'Linear Attenuation Coeff. (cm⁻¹)', data: [], borderColor: 'var(–primary-color)', backgroundColor: 'rgba(0, 74, 153, 0.2)', fill: false, yAxisID: 'y-axis-attenuation', tension: 0.1 }, { label: 'Density (g/cm³)', data: [], borderColor: 'var(–success-color)', backgroundColor: 'rgba(40, 167, 69, 0.2)', fill: false, yAxisID: 'y-axis-density', tension: 0.1 } ] }; function initializeChart() { var ctx = document.getElementById('attenuationChart').getContext('2d'); attenuationChart = new Chart(ctx, { type: 'line', data: chartData, options: { responsive: true, maintainAspectRatio: false, scales: { x: { title: { display: true, text: 'Material (Effective Z)' } }, 'y-axis-attenuation': { type: 'linear', position: 'left', title: { display: true, text: 'Attenuation Coefficient (cm⁻¹)' }, grid: { drawOnChartArea: true, }, ticks: { beginAtZero: true } }, 'y-axis-density': { type: 'linear', position: 'right', title: { display: true, text: 'Density (g/cm³)' }, ticks: { beginAtZero: true } } }, plugins: { title: { display: true, text: 'Material Properties vs. Effective Z' }, tooltip: { mode: 'index', intersect: false, } }, hover: { mode: 'index', intersect: false } } }); } function updateChart(calculatedMu, densityFactor) { if (!attenuationChart) { initializeChart(); } var detectorMaterialSelect = document.getElementById('detectorMaterial'); var selectedIndex = detectorMaterialSelect.selectedIndex; var selectedOption = detectorMaterialSelect.options[selectedIndex]; // Add current calculated data point var label = selectedOption.text.split(' (')[0]; // e.g., "Cerium Bromide" var currentZ = parseFloat(detectorMaterialSelect.value); var currentDensity = densityFactor; // Using densityInfluence as a proxy for density var currentMu = calculatedMu; // Add data if it doesn't exist, or update if it does var existingIndex = chartData.labels.indexOf(label); if (existingIndex === -1) { chartData.labels.push(label); chartData.datasets[0].data.push(currentMu); chartData.datasets[1].data.push(currentDensity); } else { chartData.datasets[0].data[existingIndex] = currentMu; chartData.datasets[1].data[existingIndex] = currentDensity; } // Add some reference data points for context if not already there var referenceData = [ { label: "Water", Z: 7.4, Density: 1.0, Mu: 0.20 }, { label: "Fat", Z: 6.5, Density: 0.92, Mu: 0.19 }, { label: "Muscle", Z: 7.4, Density: 1.06, Mu: 0.21 }, { label: "Bone", Z: 13.8, Density: 1.85, Mu: 0.45 }, ]; for (var i = 0; i < referenceData.length; i++) { var ref = referenceData[i]; var refLabel = ref.label; existingIndex = chartData.labels.indexOf(refLabel); if (existingIndex === -1) { chartData.labels.push(refLabel); chartData.datasets[0].data.push(ref.Mu); chartData.datasets[1].data.push(ref.Density); } else { // Update existing reference data if needed (less likely) chartData.datasets[0].data[existingIndex] = ref.Mu; chartData.datasets[1].data[existingIndex] = ref.Density; } } attenuationChart.update(); } // Initialize chart on page load window.onload = function() { // Pre-fill with default values for the chart to show something initially var defaultDetectorZ = parseFloat(document.getElementById('detectorMaterial').value); var defaultDensityInfluence = 1.0; // Placeholder value if (defaultDetectorZ === 14.2) defaultDensityInfluence = 1.2; if (defaultDetectorZ === 10.8) defaultDensityInfluence = 1.5; if (defaultDetectorZ === 9.5) defaultDensityInfluence = 0.9; if (defaultDetectorZ === 7.1) defaultDensityInfluence = 1.1; updateChart(0.20, defaultDensityInfluence); // Use a base Mu for initial display // Add event listeners for inputs to trigger calculation dynamically var inputs = document.querySelectorAll('.loan-calc-container input, .loan-calc-container select'); for (var i = 0; i < inputs.length; i++) { inputs[i].addEventListener('input', function() { // Delay calculation slightly to avoid performance issues during rapid typing setTimeout(calculateCTWeight, 100); }); } // Also trigger on select change document.getElementById('detectorMaterial').addEventListener('change', function() { setTimeout(calculateCTWeight, 100); }); // Add click listener for FAQ toggles var faqQuestions = document.querySelectorAll('.faq-question'); for (var i = 0; i < faqQuestions.length; i++) { faqQuestions[i].addEventListener('click', function() { var faqItem = this.parentElement; faqItem.classList.toggle('open'); }); } };

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