Magnetism and Magnetic Effects: Diagram-Based Questions (5)

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Question

A long straight wire carries current I=5 AI = 5\text{ A} along the +x+x-axis. Point PP is at (0,0.1 m,0)(0, 0.1\text{ m}, 0). Find the magnitude and direction of the magnetic field at PP.

Solution — Step by Step

For a long straight wire, the magnetic field at perpendicular distance rr is:

B=μ0I2πrB = \frac{\mu_0 I}{2\pi r}

B=4π×107×52π×0.1=2×107×50.1=105 TB = \frac{4\pi \times 10^{-7} \times 5}{2\pi \times 0.1} = \frac{2 \times 10^{-7} \times 5}{0.1} = 10^{-5}\text{ T}

Point thumb along +x+x (direction of current). Fingers curl from +y+y towards +z+z at point PP. So at (0,0.1,0)(0, 0.1, 0), the field points in the +z+z direction.

Final answer: B=105z^ T\vec{B} = 10^{-5}\,\hat{z}\text{ T}, magnitude 10μT10\,\mu\text{T}.

Why This Works

The Biot-Savart law integrated along an infinite wire gives the simple 1/r1/r falloff. The field forms concentric circles around the wire — the right-hand rule tells us which way they go. At any point in space, B\vec{B} is tangent to the circle through that point, perpendicular to both the wire and the radial vector from the wire to the point.

For finite wires, the formula gets a (sinθ1+sinθ2)/2(\sin\theta_1 + \sin\theta_2)/2 correction factor where θ1,θ2\theta_1, \theta_2 are angles to the wire ends. For “long” wires, both angles approach 90°90° and we get the formula above.

Alternative Method

Vector form of Biot-Savart:

dB=μ04πIdl×r^r2d\vec{B} = \frac{\mu_0}{4\pi}\frac{I\, d\vec{l} \times \hat{r}}{r^2}

For an element dl=dxx^d\vec{l} = dx\,\hat{x} and r^\hat{r} from the element to PP, the cross product points in +z+z when PP is in the +y+y direction. Integrating from -\infty to \infty gives the same magnitude.

Memorise: μ02π=2×107 T⋅m/A\dfrac{\mu_0}{2\pi} = 2 \times 10^{-7}\text{ T·m/A}. Then B=(2×107)I/rB = (2 \times 10^{-7})\,I/r in SI units. For I=1 AI = 1\text{ A} at r=1 mr = 1\text{ m}, B=0.2μTB = 0.2\,\mu\text{T} — earth’s field is ~50 μT for comparison.

Common Mistake

Confusing the right-hand rule for a straight wire (thumb along current, fingers curl) with the rule for a loop (fingers curl with current, thumb gives north). Both are right-hand rules, but applied differently. Practice both on simple cases until they’re automatic.

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