Moving Charges and Magnetism Lecture Notes

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Flashcards defining key concepts, formulas, and laws of magnetic fields produced by electric currents and moving charges.

Last updated 6:45 PM on 9/23/26
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17 Terms

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Oersted's Experiment

An experiment demonstrating that an electric current produces a magnetic field around a conductor, which causes a magnetic needle to deflect depending on the current's magnitude and direction.

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Magnetic Field Intensity

A vector quantity representing the strength and direction of a magnetic field at any point in space.

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Current Element Direction

The spatial vector direction of a current element dl⃗d\vec{l}, defined to be in the exact same direction as the electric current at that point.

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Magnetic Field along Wire Length

The condition where the magnetic field at any observation point located directly along the extended length line of a straight current-carrying wire is always zero (B=0B = 0).

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Magnetic Field Lines of Straight Conductor

Concentric circles formed in a plane perpendicular to a straight current-carrying wire.

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Magnetic Field of Infinitely Long Straight Wire

The magnetic field at distance dd from an infinitely long current-carrying wire, expressed as B=μ0I2πdB = \frac{\mu_0 I}{2\pi d}, showing that B∝1dB \propto \frac{1}{d}.

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Magnetic Field of Semi-Infinitely Long Wire

The field at a point near one end of a semi-infinitely long wire, given by B=μ0I4πdB = \frac{\mu_0 I}{4\pi d}.

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Magnetic Field on Perpendicular Bisector of Finite Wire

The magnetic field produced by a wire of length LL at a point on its perpendicular bisector at distance aa, given by B=μ0IL2πa4a2+L2B = \frac{\mu_0 I L}{2\pi a \sqrt{4a^2 + L^2}}.

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Magnetic Field at Centre of Arc

The magnetic field produced at the center of a circular arc subtending angle α\alpha in radians, given by B=μ0Iα4πRB = \frac{\mu_0 I \alpha}{4\pi R}.

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Magnetic Field at Centre of Circular Loop

The magnetic field at the center of a circular coil with NN turns and radius RR, given by B=μ0NI2RB = \frac{\mu_0 N I}{2R}.

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Magnetic Field at Centre of Semicircular Loop

The magnetic field generated at the center of a semicircular current loop, given by B=μ0I4RB = \frac{\mu_0 I}{4R}.

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Magnetic Field at Centre of Quarter Circle Loop

The magnetic field generated at the center of a quarter circle arc carrying current II, given by B=μ0I8RB = \frac{\mu_0 I}{8R}.

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Magnetic Field on Axis of Circular Loop

The magnetic field at a distance xx along the axis of a circular coil with NN turns and radius RR, given by B=μ0NIR22(R2+x2)3/2B = \frac{\mu_0 N I R^2}{2(R^2 + x^2)^{3/2}}.

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Magnetic Field Inside an Infinite Solenoid

The uniform magnetic field inside a long solenoid far from its ends, given by B=μ0nIB = \mu_0 n I, where nn is the number of turns per unit length.

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Magnetic Field Near End of Infinite Solenoid

The magnetic field on the axis near one end of an infinitely long solenoid, given by B=μ0nI2B = \frac{\mu_0 n I}{2}.

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Magnetic Field of a Moving Single Charge

The magnetic field generated by a charge qq moving with velocity v⃗\vec{v}, given by B⃗=μ04πq(v⃗×r^)r2\vec{B} = \frac{\mu_0}{4\pi} \frac{q (\vec{v} \times \hat{r})}{r^2}.

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Ampere's Circuital Law

A fundamental law stating that the line integral of magnetic field B⃗\vec{B} around any closed path is proportional to the total current enclosed by that path, expressed as ∮B⃗⋅dl⃗=μ0I\oint \vec{B} \cdot d\vec{l} = \mu_0 I.