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Magnetic Field Derivation for a Circular Coil
📌 The magnetic field (dB) produced by a small current element (dL) on a circular coil is calculated using the Biot-Savart Law: .
📐 Due to the geometry where the slant height (AP) is perpendicular to the coil's circumference, , simplifying the field contribution to .
🔄 When resolving the vector contributions (dB) from opposite elements (like at points A and B), the components perpendicular to the axis () add up, while the components parallel to the axis () cancel each other out.
Total Magnetic Field on the Axis
🔗 The total magnetic field ($B$) is obtained by integrating the contributing component along the loop: .
🧮 Substituting (where $a$ is the radius and $R$ is the distance AP) and (the perimeter), the formula simplifies to .
📏 Expressing $R$ in terms of the axial distance $x$ and radius $a$ (), the final expression for the magnetic field on the axis at distance $x$ is .
Special Cases and Center Field
🔄 For a coil with $n$ turns, the magnetic field is multiplied by $n$: .
⚫ The magnetic field at the center of the coil is found by setting the axial distance $x=0$, resulting in the formula .
Key Points & Insights
➡️ The derivation hinges on the geometric relationship ensuring for the magnetic field contribution from each element.
➡️ Cancellation of perpendicular components () is crucial for the net field lying purely along the axis of the coil.
➡️ The magnetic field strength at the center of the coil () represents the maximum field strength generated by the loop.
📸 Video summarized with SummaryTube.com on Nov 20, 2025, 04:55 UTC
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