Step 1: Field inside a long solenoid.
For an ideal solenoid, B_inside = μ₀ n I, uniform and axial.
Step 2: Field at the axial end.
At the solenoid's end face, the field drops to roughly half: B_end ≈ (1/2) μ₀ n I, derived from summing loop contributions.
Step 3: Ratio comparison.
B_inside / B_end = (μ₀ n I) / (½ μ₀ n I) = 2.
Step 4: Physical reasoning.
Inside, all turns add constructively; at the end, only about half the turns reinforce axially.
Step 5: Conclusion.
The interior field is twice the field at the axial end.
Step 6: Additional remark.
In finite solenoids, the field tapers smoothly from the uniform central region to half-value at the ends, consistent with Ampère's law.