Step 1: Understanding the Concept:
The problem asks for the total surface current (\(I\)) flowing through a strip, given the surface current density (\(\mathbf{K}\)). Surface current density \(\mathbf{K}\) is defined as the current per unit length perpendicular to the flow. To find the total current, we need to integrate the current density over the width of the strip.
Step 2: Key Formula or Approach:
The total current \(I\) flowing through a surface is found by integrating the surface current density \(\mathbf{K}\) over the path perpendicular to the current flow. If the current flows in the x-direction and varies with y, the infinitesimal current \(dI\) through a small width \(dy\) is \(dI = K(y) \, dy\). The total current is:
\[ I = \int K(y) \, dy \]
The integration is performed over the width of the strip.
Step 3: Detailed Explanation:
1. Identify the given quantities:
The surface current density is given as \(\mathbf{K} = ae^{-y}\). The diagram indicates that the current is flowing in the positive x-direction (\(\mathbf{K} = ae^{-y} \hat{i}\)).
The current density is uniform in x but varies with y.
The strip extends from \(y=0\) to \(y=b\).
2. Set up the integral for the total current:
To find the total current \(I\) passing through the strip, we need to integrate the magnitude of the current density, \(K(y) = ae^{-y}\), over the width of the strip, which is along the y-axis from 0 to b.
\[ I = \int_{0}^{b} K(y) \, dy \]
\[ I = \int_{0}^{b} ae^{-y} \, dy \]
3. Evaluate the integral:
The constant \(a\) can be taken out of the integral.
\[ I = a \int_{0}^{b} e^{-y} \, dy \]
The integral of \(e^{-y}\) is \(-e^{-y}\).
\[ I = a \left[ -e^{-y} \right]_{0}^{b} \]
Now, apply the limits of integration:
\[ I = a \left( (-e^{-b}) - (-e^{-0}) \right) \]
Since \(e^0 = 1\):
\[ I = a (-e^{-b} + 1) \]
\[ I = a(1 - e^{-b}) \]
Step 4: Final Answer:
The associated surface current is \(a(1 - e^{-b})\). This corresponds to option (A).