Solution 2: Maximizing Induced Current
1. Material Parameters:
We are given a wire with:
- Mass: $m$
- Density: $d$
- Resistivity: $\rho$
Let the length of the wire be $l$ and its cross-sectional area be $a$.
Volume of the wire $V = \frac{m}{d}$. Also, $V = l \cdot a$.
$$ a = \frac{m}{d \cdot l} $$2. Resistance of the Loop:
The resistance $R$ of the wire is given by:
$$ R = \rho \frac{l}{a} = \rho \frac{l}{(m / dl)} = \frac{\rho d l^2}{m} $$3. Induced EMF and Current:
The loop is placed in a magnetic field $B = \beta t$. The induced EMF is determined by the rate of change of flux.
$$ \varepsilon = \frac{d\Phi}{dt} = A_{\text{loop}} \frac{dB}{dt} $$Where $A_{\text{loop}}$ is the geometric area enclosed by the wire loop (not the cross-section $a$).
$$ \frac{dB}{dt} = \beta \implies \varepsilon = A_{\text{loop}} \beta $$The induced current $I$ is:
$$ I = \frac{\varepsilon}{R} = \frac{A_{\text{loop}} \beta}{(\rho d l^2 / m)} = \frac{m \beta}{\rho d} \left( \frac{A_{\text{loop}}}{l^2} \right) $$4. Maximizing the Current:
To maximize $I$, we need to maximize the ratio $\frac{A_{\text{loop}}}{l^2}$. This is an isoperimetric problem: for a fixed perimeter $l$, which shape encloses the maximum area?
The shape that maximizes area for a given perimeter is a Circle.
For a circle of perimeter $l$:
$$ l = 2\pi r \implies r = \frac{l}{2\pi} $$ $$ A_{\text{loop}} = \pi r^2 = \pi \left( \frac{l}{2\pi} \right)^2 = \frac{l^2}{4\pi} $$5. Final Calculation:
Substitute the maximum area ratio back into the current equation:
$$ I_{\text{max}} = \frac{m \beta}{\rho d} \left( \frac{1}{4\pi} \right) = \frac{\beta m}{4\pi \rho d} $$