Chapter 28 Physics

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Last updated 4:59 PM on 10/19/25
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14 Terms

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Biot-Savart Law

Describes the differential magnetic field created by a current element (idsids) as: dB=μ04πidssinθr2dB = \frac{\mu_0}{4\pi}\cdot \frac{ids\sin\theta}{r^2}

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Magnetic Permeability of Free Space (μ0\mu_0)

A fundamental constant with a numerical value of 4π×107 Tm/A4\pi \times 10^{-7} \text{ Tm/A}.

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Magnetic Field from a Long, Straight Wire (Magnitude)

The equation for the magnitude of the magnetic field at a distance dd from a straight wire carrying current ii is: B=μ0i2πdB = \frac{\mu_0 i}{2\pi d}

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Right-Hand Rule (for magnetic field direction)

If you point the thumb of your right hand in the direction of current, the curled fingers will point in the direction of the magnetic field.

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Magnetic Force between Two Parallel Wires

The force FF on a length LL of wire 2 due to wire 1 (carrying currents i<em>1i<em>1 and i</em>2i</em>2 separated by distance dd) is: F=i<em>2LB</em>1=i<em>2L(μ</em>0i12πd)F = i<em>2 L B</em>1 = i<em>2 L \left(\frac{\mu</em>0 i_1}{2\pi d}\right)

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Ampere (SI Definition)

The constant current that maintains a force of 2×107 N2 \times 10^{-7} \text{ N} per meter of length between two parallel conductors when both carry 1 A1\text{ A} of current and are separated by 1 m1\text{ m}.

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Magnetic Field at the Center of a Circular Loop

For a circular loop with current ii and radius RR, the magnitude of the magnetic field at its center is: B=μ0i2RB = \frac{\mu_0 i}{2R}

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Ampere's Law

States that the line integral of the magnetic field over a closed loop is proportional to the total current enclosed by the loop: Bds=μ<em>0i</em>enc\oint B \cdot ds = \mu<em>0 i</em>{\text{enc}}.

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Magnetic Field Inside a Solenoid

For a solenoid with nn turns per unit length carrying current ii, the uniform magnetic field inside is: B=μ0niB = \mu_0 n i.

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Magnetic Field Inside a Toroid

For a toroid with NN turns carrying current ii at a radius rr within the toroid, the magnetic field is: B=μ0Ni2πrB = \frac{\mu_0 N i}{2\pi r}.

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Diamagnetism

A property of materials with negative magnetic susceptibility (\chi_m < 0) that oppose external magnetic fields.

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Paramagnetism

A property of materials with positive magnetic susceptibility (\chi_m > 0) that show alignment under external magnetic fields.

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Ferromagnetism

A property of materials that maintain magnetic alignment even after external magnetic fields are removed.

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Curie Temperature

The critical temperature above which heating disrupts ferromagnetic alignment.