Step 1: State why the lower frequency signal delays more.
Because ionospheric delay $\Delta t = k\, TEC/f^2$ (k a constant), a smaller carrier frequency $f$ produces a larger $1/f^2$ term and hence a larger delay. Since $f_{L2} = 1227.60\ MHz$ is lower than $f_{L1} = 1575.42\ MHz$, the L2 signal must be delayed more than L1.
Step 2: Compute $1/f^2$ for each carrier.
\[ \frac{1}{f_{L1}^2} = \frac{1}{(1575.42)^2} = \frac{1}{2481941} = 4.0291\times10^{-7} \] \[ \frac{1}{f_{L2}^2} = \frac{1}{(1227.60)^2} = \frac{1}{1507005} = 6.6357\times10^{-7} \]
Step 3: Take the ratio of the two delay factors.
\[ \frac{\Delta t_{L2}}{\Delta t_{L1}} = \frac{1/f_{L2}^2}{1/f_{L1}^2} = \frac{6.6357\times10^{-7}}{4.0291\times10^{-7}} \]
Step 4: Evaluate the ratio.
\[ \frac{\Delta t_{L2}}{\Delta t_{L1}} = 1.6470 \]
Step 5: Round to the nearest integer and conclude.
\[ \frac{\Delta t_{L2}}{\Delta t_{L1}} \approx 2 \] The GPS L2 carrier is therefore delayed by roughly twice as much as the L1 carrier for the same ionospheric TEC, confirming the earlier symbolic derivation.
\[ \boxed{\text{Factor} \approx 2} \]