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:
\[
\boxed{2.50 \, A/m}
\]
Given an open-loop transfer function \(GH = \frac{100}{s}(s+100)\) for a unity feedback system with a unit step input \(r(t)=u(t)\), determine the rise time \(t_r\).
Consider a linear time-invariant system represented by the state-space equation: \[ \dot{x} = \begin{bmatrix} a & b -a & 0 \end{bmatrix} x + \begin{bmatrix} 1 0 \end{bmatrix} u \] The closed-loop poles of the system are located at \(-2 \pm j3\). The value of the parameter \(b\) is: