## Student handout: Magnetic Field Due to a Spinning Ring of Charge

Static Fields 2024 (11 years)

Students work in small groups to use the Biot-Savart law $\vec{B}(\vec{r}) =\frac{\mu_0}{4\pi}\int\frac{\vec{J}(\vec{r}^{\,\prime})\times \left(\vec{r}-\vec{r}^{\,\prime}\right)}{\vert \vec{r}-\vec{r}^{\,\prime}\vert^3} \, d\tau^{\prime}$ to find an integral expression for the magnetic field, $\vec{B}(\vec{r})$, due to a spinning ring of charge.

In an optional extension, students find a series expansion for $\vec{B}(\vec{r})$ either on the axis or in the plane of the ring, for either small or large values of the relevant geometric variable. Add an extra half hour or more to the time estimate for the optional extension.

• group Small Group Activity schedule 30 min. build whiteboards/markers/erasers, hula hoop, coordinate axes on the ceiling description Student handout (PDF)
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What students learn
• to perform a magnetic field calculation using the Biot-Savart Law;
• to decide which form of the Biot-Savart Law to use, depending on the dimensions of the current density;
• how to find current from total charge $Q$, period $T$, and the geometry of the problem, radius $R$;
• to perform the cross product in the numerator of the Biot-Savart Law using cyclindrical basis vectors;
• to write the distance formula $\vec{r}-\vec{r'}$ in both the numerator and denominator of the Biot-Savart Law in an appropriate mix of cylindrical coordinates and rectangular basis vectors;
The Magnetic Field Due to a Spinning Ring of Charge
1. Use the Biot-Savart law $\vec{B}(\vec{r}) =\frac{\mu_0}{4\pi}\int\frac{\vec{J}(\vec{r}^{\,\prime})\times \left(\vec{r}-\vec{r}^{\,\prime}\right)}{\vert \vec{r}-\vec{r}^{\,\prime}\vert^3} \, d\tau^{\prime}$ to find the magnetic field everywhere in space due to a spinning charged ring with radius $R$, total charge $Q$, and period $T$.
2. Evaluate your expression for the special case that $\vec{r}$ is on the $z$-axis.
3. Evaluate your expression for the special case that $\vec{r}$ is on the $x$-axis.
4. Find a series expansion for the electrostatic potential at these special locations:
1. Near the center of the ring, in the plane of the ring;
2. Near the center of the ring, on the axis of the ring;
3. Far from the ring on the axis of symmetry;
4. Far from the ring, in the plane of the ring.

Author Information
Corinne Manogue, Leonard Cerny
Keywords

Learning Outcomes