An inductor with resistance acts as a series combination of a pure inductor ($L$) and a resistor ($R$). When the circuit is closed, the rate of change of current determines the voltage across the inductor portion. The governing equation for the circuit is:
$$ L \frac{di}{dt} + iR = E $$
The voltage across the inductor is specifically the induced EMF, which is $V_L = L \frac{di}{dt}$. From the circuit equation, we can see that:
$$ V_L = E - iR $$
Given parameters:
$E = 1.0 \text{ V}$
$R = 100 \text{ } \Omega$
Step 1: Calculate the voltage for the first current value.
For $i = 2 \text{ mA} = 0.002 \text{ A}$:
$$ V_1 = 1 - (0.002)(100) = 1 - 0.2 = 0.8 \text{ V} $$
Step 2: Calculate the voltage for the second current value.
For $i = 4 \text{ mA} = 0.004 \text{ A}$:
$$ V_2 = 1 - (0.004)(100) = 1 - 0.4 = 0.6 \text{ V} $$
Step 3: Find the ratio between the two calculated voltages.
$$ \frac{V_1}{V_2} = \frac{0.8}{0.6} $$
By simplifying the fraction by dividing both numerator and denominator by $0.2$, we get:
$$ \frac{V_1}{V_2} = \frac{4}{3} $$
The ratio is $4/3$, matching option 1.