Step 1: Write the first-order ionospheric delay relation.
The ionospheric time delay experienced by a GNSS signal follows \[ \Delta t \propto \frac{TEC}{f^2} \] for a fixed Total Electron Content (TEC), so the delay on any carrier is inversely proportional to the square of its frequency.
Step 2: Set up the ratio of delays for L2 and L1.
Since TEC is the same for both signals (they pass through essentially the same ionospheric path), \[ \frac{\Delta t_{L2}}{\Delta t_{L1}} = \frac{1/f_{L2}^2}{1/f_{L1}^2} = \left(\frac{f_{L1}}{f_{L2}}\right)^2 \]
Step 3: Substitute the carrier frequencies.
\(f_{L1} = 1575.42\ MHz\) and \(f_{L2} = 1227.60\ MHz\): \[ \frac{f_{L1}}{f_{L2}} = \frac{1575.42}{1227.60} = 1.28333 \]
Step 4: Square the frequency ratio.
\[ \left(\frac{f_{L1}}{f_{L2}}\right)^2 = (1.28333)^2 = 1.64694 \]
Step 5: Round off to the nearest integer.
\[ \frac{\Delta t_{L2}}{\Delta t_{L1}} \approx 1.647 \approx 2 \] So the L2 carrier, being at the lower frequency, is delayed (slowed) by a factor of about \(2\) relative to L1 for the same TEC, matching the accepted answer.
\[ \boxed{\text{Factor} \approx 2} \]