Calculate Resistors in Parallel

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Calculate Resistors in Parallel

Parallel Resistor Calculator

Enter the resistance value for the first resistor in Ohms (Ω).
Enter the resistance value for the second resistor in Ohms (Ω).
Enter the resistance value for the third resistor in Ohms (Ω). (Optional)
Enter the resistance value for the fourth resistor in Ohms (Ω). (Optional)
Enter the resistance value for the fifth resistor in Ohms (Ω). (Optional)

Calculation Results

— Ω

Reciprocal of R1:

Reciprocal of R2:

Reciprocal of R3:

Reciprocal of R4:

Reciprocal of R5:

Sum of Reciprocals:

Formula Used: The total equivalent resistance (Req) of resistors connected in parallel is the reciprocal of the sum of the reciprocals of individual resistances.

1 / Req = 1 / R1 + 1 / R2 + 1 / R3 + … + 1 / Rn

Therefore, Req = 1 / (1 / R1 + 1 / R2 + 1 / R3 + … + 1 / Rn)

Resistance Values Used
Resistor Resistance (Ω) Reciprocal (1/Ω)
R1
R2
R3
R4
R5
Total Equivalent (Req)

Parallel Resistance Visualization

Individual Resistance Equivalent Resistance

What is Parallel Resistance Calculation?

Understanding how to calculate resistors in parallel is a fundamental concept in electronics and electrical engineering. When components are connected in parallel, they offer multiple paths for current to flow. This configuration is distinct from a series connection, where components are connected end-to-end, providing only a single path for current. Calculating the total equivalent resistance of a parallel circuit is crucial for designing and troubleshooting electronic devices, ensuring proper current distribution, and predicting circuit behavior.

Who Should Use This Calculator?

This calculator is an invaluable tool for a wide range of individuals, including:

  • Students: Electrical engineering, physics, and electronics students learning about circuit analysis.
  • Hobbyists: Electronics enthusiasts working on DIY projects, breadboarding circuits, or building custom devices.
  • Technicians: Field technicians and repair personnel troubleshooting electronic equipment.
  • Engineers: Design engineers selecting appropriate components and verifying circuit performance.
  • Educators: Teachers demonstrating circuit principles and providing practical examples.

Common Misconceptions About Parallel Resistors

Several common misunderstandings can arise when dealing with parallel resistors:

  • Misconception 1: The total resistance is simply the sum of individual resistances. This is true for series circuits, but for parallel circuits, the total resistance is always *less* than the smallest individual resistance.
  • Misconception 2: Adding more resistors in parallel increases the total resistance. In reality, adding more resistors in parallel *decreases* the total equivalent resistance because it provides more paths for current.
  • Misconception 3: The voltage across each parallel resistor is different. In a parallel circuit, the voltage across each branch is the same.

This calculator helps to demystify these concepts by providing accurate, real-time calculations.

Parallel Resistance Formula and Mathematical Explanation

The core principle behind calculating resistors in parallel lies in the concept of conductance, which is the reciprocal of resistance (G = 1/R). In a parallel circuit, the total conductance is the sum of the individual conductances.

Step-by-Step Derivation

Consider a circuit with 'n' resistors (R1, R2, R3, …, Rn) connected in parallel across a voltage source.

  1. Kirchhoff's Current Law (KCL): The total current (Itotal) entering the parallel combination is the sum of the currents flowing through each individual resistor (I1, I2, …, In).
    Itotal = I1 + I2 + … + In
  2. Ohm's Law: For each resistor, the current is given by Ohm's Law (I = V/R). Since all resistors are in parallel, the voltage (V) across each is the same.
    I1 = V / R1
    I2 = V / R2

    In = V / Rn
  3. Substitution: Substitute these expressions for individual currents back into KCL.
    Itotal = (V / R1) + (V / R2) + … + (V / Rn)
  4. Factoring out Voltage: Factor out the common voltage V.
    Itotal = V * (1 / R1 + 1 / R2 + … + 1 / Rn)
  5. Total Equivalent Resistance (Req): We also know from Ohm's Law that Itotal = V / Req. Equating this with the previous expression:
    V / Req = V * (1 / R1 + 1 / R2 + … + 1 / Rn)
  6. Simplification: Divide both sides by V (assuming V is not zero).
    1 / Req = 1 / R1 + 1 / R2 + … + 1 / Rn
  7. Final Formula: To find Req, take the reciprocal of both sides.
    Req = 1 / (1 / R1 + 1 / R2 + … + 1 / Rn)

Variable Explanations

Here's a breakdown of the variables involved in the parallel resistance calculation:

Parallel Resistance Variables
Variable Meaning Unit Typical Range
R1, R2, …, Rn Resistance of individual resistors Ohms (Ω) 0.1 Ω to several Megaohms (MΩ)
Req Total equivalent resistance of the parallel combination Ohms (Ω) Less than the smallest individual R
1 / R Conductance of an individual resistor Siemens (S) or mhos Varies based on R
Sum of Reciprocals Total conductance of the parallel network Siemens (S) Varies based on R values

Practical Examples (Real-World Use Cases)

Let's illustrate the calculation with practical scenarios:

Example 1: Simple LED Circuit

Suppose you want to power two LEDs in parallel, each requiring a specific current limiting resistor. Let's say you have two identical LEDs, and you want to connect them in parallel to a 5V source. Each LED has a forward voltage drop of 2V and requires a current of 20mA (0.02A). You need to calculate the resistance for each branch.

Scenario: Two parallel branches, each with an LED and a current-limiting resistor.

Inputs:

  • Voltage Source (V): 5V
  • LED Forward Voltage (Vf): 2V
  • Desired Current per LED (If): 0.02A

Calculation for one branch's resistor (R_limit):

The voltage across the resistor is V_resistor = V_source – Vf = 5V – 2V = 3V.

Using Ohm's Law (R = V/I): R_limit = V_resistor / If = 3V / 0.02A = 150Ω.

Now, if we were to connect these two *resistors* (R_limit = 150Ω each) in parallel (perhaps as part of a more complex network), the total resistance of just these two resistors would be:

1 / Req = 1 / 150Ω + 1 / 150Ω = 0.00667 S + 0.00667 S = 0.01334 S

Req = 1 / 0.01334 S ≈ 75Ω

Interpretation: The total resistance of the two 150Ω resistors in parallel is 75Ω, which is less than the smallest individual resistance (150Ω). This demonstrates how parallel paths reduce overall resistance.

Example 2: Voltage Divider Network

Consider a scenario where you need to create a specific voltage output using a voltage divider, which often involves resistors in parallel to achieve a precise resistance value.

Scenario: You need a total resistance of 50Ω for a specific part of a circuit. You have a 100Ω resistor and a 100Ω resistor available.

Inputs:

  • Resistor 1 (R1): 100Ω
  • Resistor 2 (R2): 100Ω

Calculation using the calculator:

1 / Req = 1 / 100Ω + 1 / 100Ω = 0.01 S + 0.01 S = 0.02 S

Req = 1 / 0.02 S = 50Ω

Interpretation: By connecting two 100Ω resistors in parallel, you achieve a combined resistance of 50Ω. This is a common technique to obtain resistance values not readily available as single components or to handle higher power dissipation by sharing the load.

How to Use This Parallel Resistor Calculator

Using our calculator is straightforward and designed for efficiency:

  1. Enter Resistance Values: Input the resistance values (in Ohms, Ω) for each resistor you wish to connect in parallel into the respective fields (Resistor 1, Resistor 2, etc.). You can calculate for up to five resistors.
  2. Optional Fields: Fields for Resistor 3, 4, and 5 are optional. If you only have two resistors, simply leave the others blank or ensure they are set to a default value that won't affect the calculation if they are not intended to be part of the circuit (though the calculator handles zero or empty inputs gracefully by ignoring them in the sum of reciprocals).
  3. Calculate: Click the "Calculate Total Resistance" button.
  4. View Results: The calculator will instantly display:
    • The Total Equivalent Resistance (Req) in Ohms (Ω), prominently displayed.
    • The reciprocal value (conductance) for each entered resistor.
    • The sum of all reciprocals (total conductance).
    • A clear explanation of the formula used.
  5. Review Table: Examine the table below the calculator for a detailed breakdown of individual resistances and their reciprocals, along with the final equivalent resistance.
  6. Visualize: Observe the bar chart, which visually compares the individual resistance values against the calculated equivalent resistance. Notice how the equivalent resistance is always lower than the smallest individual resistance.
  7. Copy Results: Use the "Copy Results" button to easily transfer the key calculation outputs to your notes or reports.
  8. Reset: Click "Reset Defaults" to clear all fields and return them to their initial example values.

Decision-Making Guidance: The primary use is to determine the combined resistance of parallel components. This is vital for ensuring circuits operate within design parameters, managing current flow, and preventing component damage. For instance, if a circuit requires a specific resistance value that isn't available, you can use this calculator to find combinations of available resistors that achieve the target value.

Key Factors That Affect Parallel Resistance Results

While the formula for parallel resistors is precise, several real-world factors can influence the actual performance and interpretation of results:

  1. Resistor Tolerance: Real resistors are not manufactured to exact values; they have a tolerance (e.g., ±5%, ±1%). This means the actual resistance might deviate slightly from the nominal value, leading to a slightly different equivalent resistance than calculated. Always consider the tolerance range when precision is critical.
  2. Temperature Coefficients: The resistance of most materials changes with temperature. If the resistors operate in a high-temperature environment or experience significant self-heating due to current flow, their resistance values can drift, affecting the overall circuit resistance.
  3. Parasitic Inductance and Capacitance: At very high frequencies, the physical characteristics of resistors (like lead inductance and internal capacitance) become significant. These parasitic elements can alter the effective impedance of the resistor, deviating from its purely resistive value and impacting the parallel combination's behavior.
  4. Connection Resistance: The resistance of wires, solder joints, or connectors used to link the resistors in parallel adds a small amount of resistance to the circuit. While often negligible in low-power circuits, it can become significant in high-current applications or when dealing with very low resistance values.
  5. Power Dissipation Limits: Each resistor has a maximum power rating (in Watts). When resistors are in parallel, the total current is divided among them. While this often reduces the power dissipated by each individual resistor compared to a series circuit, you must ensure that the power rating of each resistor is not exceeded, considering the total current and the resistance of each branch. The total power dissipated by the parallel combination is the sum of the power dissipated by each resistor.
  6. Component Aging: Over long periods, resistors can degrade due to environmental factors or electrical stress, leading to changes in their resistance value. This gradual change can alter the performance of the circuit over time.

Frequently Asked Questions (FAQ)

Q1: What happens if I enter a resistance of 0 Ohms?
A: Entering 0 Ohms for a resistor in parallel effectively creates a short circuit. Mathematically, the reciprocal of 0 is undefined (approaches infinity). In a practical circuit, this would cause the total equivalent resistance to become 0 Ohms, as all current would flow through the zero-resistance path, potentially damaging the power source or other components. Our calculator will handle this by showing an error or a result tending towards zero.

Q2: Can I use this calculator for more than five resistors?
A: This specific calculator is designed for up to five resistors. For circuits with more resistors, you would simply extend the formula: 1 / Req = 1 / R1 + 1 / R2 + … + 1 / Rn + 1 / R(n+1) + … . The principle remains the same.

Q3: Is the total resistance in parallel always less than the smallest resistor?
A: Yes, assuming all individual resistances are positive values. Adding more parallel paths provides more routes for current to flow, effectively reducing the overall opposition to current. The equivalent resistance will approach zero as more resistors are added or as individual resistances become smaller.

Q4: What is the difference between parallel and series resistance calculation?
A: In a series circuit, resistances add up directly: R_total = R1 + R2 + … . The total resistance is always greater than any individual resistance. In a parallel circuit, the reciprocal of the total resistance is the sum of the reciprocals of individual resistances: 1/R_total = 1/R1 + 1/R2 + … . The total resistance is always less than the smallest individual resistance.

Q5: How does conductance relate to parallel resistors?
A: Conductance (G = 1/R) is the inverse of resistance and measures how easily current flows. For parallel resistors, the total conductance is simply the sum of the individual conductances: G_total = G1 + G2 + … . This makes the calculation conceptually simpler: add the conductances, then take the reciprocal to find the equivalent resistance.

Q6: What if I have a mix of series and parallel components?
A: You would need to simplify the circuit in stages. First, calculate the equivalent resistance for any parallel sections. Then, treat these equivalent resistances as single resistors and combine them with any other series components. Repeat this process until the entire circuit is reduced to a single equivalent resistance.

Q7: Does the calculator account for power ratings?
A: No, this calculator only determines the equivalent resistance value. It does not consider the power rating (Wattage) of the individual resistors. You must ensure that each resistor used in a parallel combination is rated to handle the power it will dissipate based on the current flowing through it and its resistance (P = I²R = V²/R).

Q8: Can I use negative resistance values?
A: Negative resistance is a concept used in specific active electronic circuits (like oscillators) and is not applicable to standard passive resistor calculations. This calculator expects positive resistance values in Ohms.

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var canvas = document.getElementById('resistanceChart'); var ctx = canvas.getContext('2d'); var chartData = { labels: [], datasets: [{ label: 'Individual Resistance (Ω)', data: [], backgroundColor: 'rgba(0, 74, 153, 0.6)', borderColor: 'rgba(0, 74, 153, 1)', borderWidth: 1 }, { label: 'Equivalent Resistance (Ω)', data: [], backgroundColor: 'rgba(40, 167, 69, 0.6)', borderColor: 'rgba(40, 167, 69, 1)', borderWidth: 1 }] }; var resistanceChart = new Chart(ctx, { type: 'bar', data: chartData, options: { responsive: true, maintainAspectRatio: false, scales: { y: { beginAtZero: true, title: { display: true, text: 'Resistance (Ohms)' } }, x: { title: { display: true, text: 'Resistor' } } }, plugins: { legend: { display: false // Using custom legend below canvas }, title: { display: true, text: 'Comparison of Individual vs. Equivalent Resistance' } } } }); function updateChart(resistors) { var labels = []; var individualData = []; var equivalentData = []; var maxIndividualResistance = 0; for (var i = 0; i maxIndividualResistance) { maxIndividualResistance = parseFloat(rVal); } } } var totalReq = calculateTotalResistanceInternal(resistors); if (totalReq !== null && totalReq > 0) { // Add equivalent resistance as a single bar or line for comparison // For simplicity, let's add it as a separate dataset entry if needed, // or just ensure the Y-axis scale accommodates it. // Here, we'll just ensure the scale is appropriate and maybe add a line later if needed. // For a bar chart, comparing individual bars to a single Req bar can be tricky. // Let's adjust the approach: show individual bars and a marker for Req. // Or, simpler: just ensure the Y-axis is sufficient. // Let's make the equivalent resistance a distinct bar if there are multiple resistors. if (labels.length > 0) { labels.push('Req'); individualData.push(null); // Placeholder for Req in individual series equivalentData.push(totalReq); } else { // Only Req exists labels.push('Req'); individualData.push(null); equivalentData.push(totalReq); } } else if (totalReq === 0) { // Handle short circuit case visually if needed labels.push('Req'); individualData.push(null); equivalentData.push(0); } else { // No valid resistors entered or calculation failed labels.push('N/A'); individualData.push(null); equivalentData.push(null); } chartData.labels = labels; chartData.datasets[0].data = individualData; chartData.datasets[1].data = equivalentData; // Adjust Y-axis scale if necessary var maxY = maxIndividualResistance > 0 ? maxIndividualResistance : 100; // Default max if no resistors if (totalReq !== null && totalReq > 0) { maxY = Math.max(maxY, totalReq); } // Add some padding to the top of the Y-axis var yAxisMax = maxY * 1.15; if (yAxisMax === 0) yAxisMax = 1; // Ensure minimum scale resistanceChart.options.scales.y.max = yAxisMax; resistanceChart.update(); } function validateInput(inputId, errorId, minValue = 0) { var input = document.getElementById(inputId); var errorElement = document.getElementById(errorId); var value = input.value.trim(); var numValue = parseFloat(value); errorElement.textContent = "; // Clear previous error if (value === ") { // Allow empty for optional fields, but error if it's the only one and calculation fails return true; // Consider empty valid for now, calculation logic will handle } if (isNaN(numValue)) { errorElement.textContent = 'Please enter a valid number.'; return false; } if (numValue < minValue) { errorElement.textContent = 'Value cannot be negative.'; return false; } return true; } function calculateTotalResistanceInternal(resistorInputs) { var sumReciprocals = 0; var validResistors = []; var hasValidInput = false; for (var i = 0; i 0) { sumReciprocals += (1 / numValue); validResistors.push({ id: input.id, value: numValue }); hasValidInput = true; } else if (value !== " && !isNaN(numValue) && numValue === 0) { // Handle zero resistance as a short circuit return 0; } } if (!hasValidInput) { return null; // No valid positive resistors entered } if (sumReciprocals === 0) { return null; // Should not happen if hasValidInput is true, but safety check } return 1 / sumReciprocals; } function calculateParallelResistance() { var resistors = [ document.getElementById('resistor1'), document.getElementById('resistor2'), document.getElementById('resistor3'), document.getElementById('resistor4'), document.getElementById('resistor5') ]; var allValid = true; var inputsToValidate = [ { id: 'resistor1', errorId: 'resistor1Error' }, { id: 'resistor2', errorId: 'resistor2Error' }, { id: 'resistor3', errorId: 'resistor3Error' }, { id: 'resistor4', errorId: 'resistor4Error' }, { id: 'resistor5', errorId: 'resistor5Error' } ]; for (var i = 0; i 0) ? (1 / r1) : null; var reciprocalR2 = (r2 > 0) ? (1 / r2) : null; var reciprocalR3 = (r3 > 0) ? (1 / r3) : null; var reciprocalR4 = (r4 > 0) ? (1 / r4) : null; var reciprocalR5 = (r5 > 0) ? (1 / r5) : null; var sumReciprocals = 0; if (reciprocalR1 !== null) sumReciprocals += reciprocalR1; if (reciprocalR2 !== null) sumReciprocals += reciprocalR2; if (reciprocalR3 !== null) sumReciprocals += reciprocalR3; if (reciprocalR4 !== null) sumReciprocals += reciprocalR4; if (reciprocalR5 !== null) sumReciprocals += reciprocalR5; var totalReq = null; if (sumReciprocals > 0) { totalReq = 1 / sumReciprocals; } else if (r1 === 0 || r2 === 0 || r3 === 0 || r4 === 0 || r5 === 0) { // Check if any input was exactly 0 var anyZero = false; if (r1 === 0 || r2 === 0 || r3 === 0 || r4 === 0 || r5 === 0) { anyZero = true; } if (anyZero) totalReq = 0; // Short circuit case } document.getElementById('reciprocalR1').textContent = reciprocalR1 !== null ? reciprocalR1.toFixed(6) : '–'; document.getElementById('reciprocalR2').textContent = reciprocalR2 !== null ? reciprocalR2.toFixed(6) : '–'; document.getElementById('reciprocalR3').textContent = reciprocalR3 !== null ? reciprocalR3.toFixed(6) : '–'; document.getElementById('reciprocalR4').textContent = reciprocalR4 !== null ? reciprocalR4.toFixed(6) : '–'; document.getElementById('reciprocalR5').textContent = reciprocalR5 !== null ? reciprocalR5.toFixed(6) : '–'; document.getElementById('sumReciprocals').textContent = sumReciprocals > 0 ? sumReciprocals.toFixed(6) : (totalReq === 0 ? 'Infinity (Short Circuit)' : '–'); var mainResultElement = document.getElementById('main-result'); if (totalReq !== null) { mainResultElement.textContent = totalReq.toFixed(2) + ' Ω'; } else { mainResultElement.textContent = '– Ω'; } updateTableAndChart(r1, r2, r3, r4, r5, reciprocalR1, reciprocalR2, reciprocalR3, reciprocalR4, reciprocalR5, totalReq, sumReciprocals); updateChart(resistors); // Update the chart with current values } function updateTableAndChart(r1, r2, r3, r4, r5, recR1, recR2, recR3, recR4, recR5, totalReq, sumReciprocals) { var tableR1 = document.getElementById('tableR1'); var tableR2 = document.getElementById('tableR2'); var tableR3 = document.getElementById('tableR3'); var tableR4 = document.getElementById('tableR4'); var tableR5 = document.getElementById('tableR5'); var tableReciprocalR1 = document.getElementById('tableReciprocalR1'); var tableReciprocalR2 = document.getElementById('tableReciprocalR2'); var tableReciprocalR3 = document.getElementById('tableReciprocalR3'); var tableReciprocalR4 = document.getElementById('tableReciprocalR4'); var tableReciprocalR5 = document.getElementById('tableReciprocalR5'); var tableTotalReq = document.getElementById('tableTotalReq'); tableR1.textContent = (r1 !== undefined && r1 !== null) ? r1.toFixed(2) : '–'; tableR2.textContent = (r2 !== undefined && r2 !== null) ? r2.toFixed(2) : '–'; tableR3.textContent = (r3 !== undefined && r3 !== null) ? r3.toFixed(2) : '–'; tableR4.textContent = (r4 !== undefined && r4 !== null) ? r4.toFixed(2) : '–'; tableR5.textContent = (r5 !== undefined && r5 !== null) ? r5.toFixed(2) : '–'; tableReciprocalR1.textContent = (recR1 !== null && recR1 !== undefined) ? recR1.toFixed(6) : '–'; tableReciprocalR2.textContent = (recR2 !== null && recR2 !== undefined) ? recR2.toFixed(6) : '–'; tableReciprocalR3.textContent = (recR3 !== null && recR3 !== undefined) ? recR3.toFixed(6) : '–'; tableReciprocalR4.textContent = (recR4 !== null && recR4 !== undefined) ? recR4.toFixed(6) : '–'; tableReciprocalR5.textContent = (recR5 !== null && recR5 !== undefined) ? recR5.toFixed(6) : '–'; if (totalReq !== null) { tableTotalReq.textContent = totalReq.toFixed(2) + ' Ω'; } else if (sumReciprocals === Infinity) { // Handle short circuit case tableTotalReq.textContent = '0 Ω (Short Circuit)'; } else { tableTotalReq.textContent = '–'; } } function resetCalculator() { document.getElementById('resistor1').value = '100'; document.getElementById('resistor2').value = '220'; document.getElementById('resistor3').value = '330'; document.getElementById('resistor4').value = '470'; document.getElementById('resistor5').value = '680'; // Clear error messages document.getElementById('resistor1Error').textContent = "; document.getElementById('resistor2Error').textContent = "; document.getElementById('resistor3Error').textContent = "; document.getElementById('resistor4Error').textContent = "; document.getElementById('resistor5Error').textContent = "; calculateParallelResistance(); // Recalculate with default values } function copyResults() { var mainResult = document.getElementById('main-result').textContent; var reciprocalR1 = document.getElementById('reciprocalR1').textContent; var reciprocalR2 = document.getElementById('reciprocalR2').textContent; var reciprocalR3 = document.getElementById('reciprocalR3').textContent; var reciprocalR4 = document.getElementById('reciprocalR4').textContent; var reciprocalR5 = document.getElementById('reciprocalR5').textContent; var sumReciprocals = document.getElementById('sumReciprocals').textContent; var tableR1 = document.getElementById('tableR1').textContent; var tableR2 = document.getElementById('tableR2').textContent; var tableR3 = document.getElementById('tableR3').textContent; var tableR4 = document.getElementById('tableR4').textContent; var tableR5 = document.getElementById('tableR5').textContent; var tableReciprocalR1 = document.getElementById('tableReciprocalR1').textContent; var tableReciprocalR2 = document.getElementById('tableReciprocalR2').textContent; var tableReciprocalR3 = document.getElementById('tableReciprocalR3').textContent; var tableReciprocalR4 = document.getElementById('tableReciprocalR4').textContent; var tableReciprocalR5 = document.getElementById('tableReciprocalR5').textContent; var tableTotalReq = document.getElementById('tableTotalReq').textContent; var resultsText = "Parallel Resistor Calculation Results:\n\n"; resultsText += "Total Equivalent Resistance (Req): " + mainResult + "\n\n"; resultsText += "Intermediate Values:\n"; resultsText += " Reciprocal R1: " + reciprocalR1 + "\n"; resultsText += " Reciprocal R2: " + reciprocalR2 + "\n"; resultsText += " Reciprocal R3: " + reciprocalR3 + "\n"; resultsText += " Reciprocal R4: " + reciprocalR4 + "\n"; resultsText += " Reciprocal R5: " + reciprocalR5 + "\n"; resultsText += " Sum of Reciprocals: " + sumReciprocals + "\n\n"; resultsText += "Detailed Breakdown:\n"; resultsText += " R1: " + tableR1 + " Ω\n"; resultsText += " R2: " + tableR2 + " Ω\n"; resultsText += " R3: " + tableR3 + " Ω\n"; resultsText += " R4: " + tableR4 + " Ω\n"; resultsText += " R5: " + tableR5 + " Ω\n"; resultsText += " Reciprocal R1: " + tableReciprocalR1 + "\n"; resultsText += " Reciprocal R2: " + tableReciprocalR2 + "\n"; resultsText += " Reciprocal R3: " + tableReciprocalR3 + "\n"; resultsText += " Reciprocal R4: " + tableReciprocalR4 + "\n"; resultsText += " Reciprocal R5: " + tableReciprocalR5 + "\n"; resultsText += " Total Equivalent Req: " + tableTotalReq + "\n\n"; resultsText += "Formula Used: 1 / Req = 1 / R1 + 1 / R2 + … + 1 / Rn"; // Use navigator.clipboard for modern browsers, fallback to textarea 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); } } 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 ? 'Results copied to clipboard!' : 'Failed to copy results.'; alert(msg); } catch (err) { console.error('Fallback: Oops, unable to copy', err); alert('Failed to copy results.'); } document.body.removeChild(textArea); } // Initial calculation on page load document.addEventListener('DOMContentLoaded', function() { calculateParallelResistance(); // Add event listeners for real-time updates var inputs = document.querySelectorAll('.loan-calc-container input[type="number"]'); for (var i = 0; i < inputs.length; i++) { inputs[i].addEventListener('input', calculateParallelResistance); } });

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