Step 1: Understanding the Concept:
The magnetic field at the centroid of a current-carrying polygon is the sum of the fields produced by each individual side. For an equilateral triangle, all three sides contribute equally and in the same direction.
Step 2: Key Formula or Approach:
1. Field due to a finite straight wire: \(B = \frac{\mu_0 I}{4\pi r} (\sin \theta_1 + \sin \theta_2)\).
2. For equilateral triangle side \(a\), distance to centroid \(r = \frac{a}{2\sqrt{3}}\) and \(\theta_1 = \theta_2 = 60^{\circ}\).
Step 3: Detailed Explanation:
Given \(I = 1.5\,\text{A}\), \(a = 0.09\,\text{m}\).
Field due to one side:
\[ B_1 = \frac{10^{-7} \times 1.5}{0.09 / (2\sqrt{3})} (\sin 60^{\circ} + \sin 60^{\circ}) \]
\[ B_1 = \frac{10^{-7} \times 1.5 \times 2\sqrt{3}}{0.09} (\sqrt{3}) = \frac{10^{-7} \times 1.5 \times 6}{0.09} = 10^{-5}\,\text{T} \]
Total field at centroid \(B = 3 \times B_1 = 3 \times 10^{-5}\,\text{T}\).
Direction: Since the current is clockwise, by the right-hand thumb rule, the magnetic field at the center points into (inside) the plane of the triangle.
Step 4: Final Answer:
The magnetic field is \(3 \times 10^{-5}\) T, inside the plane.