Step 1: Recall boundary condition.
For a surface current density \(K\) (A/m) on a sheet, the magnetic field intensity \(H\) is given by:
\[
\hat{n} \times (H_{above} - H_{below}) = K
\]
where \(\hat{n}\) is the normal vector to the surface.
Step 2: Geometry.
Here, surface = x–y plane, so normal vector is \(\hat{a}_z\).
Surface current density: \(K = 5 \hat{a}_x \, A/m\).
Step 3: Relation.
\[
H_{above} - H_{below} = K \times \hat{n}
\]
\[
= (5\hat{a}_x) \times \hat{a}_z
\]
\[
= 5(-\hat{a}_y)
\]
Step 4: Symmetry.
The field splits equally above and below the sheet:
\[
H_{above} = -\tfrac{1}{2} K \times \hat{n} = 2.5 \hat{a}_y
\]
Magnitude:
\[
|H| = 2.5 \, A/m
\]
Final Answer:
\[
\boxed{2.50 \, A/m}
\]
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