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A current of 2A is flowing in the sides of an equilateral triangle of side 9 cm. The magnetic field at the centroid of the triangle is

A

`1.66xx10^(-6)T`

B

`1.22xx10^(-4)T`

C

`1.33xx10^(-6)T`

D

`1.44xx10^(-4)T`

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To find the magnetic field at the centroid of an equilateral triangle with a current flowing through its sides, we can follow these steps: ### Step 1: Understand the Geometry of the Triangle We have an equilateral triangle ABC with each side measuring 9 cm. The centroid (O) of the triangle is the point where all three medians intersect. The distance from the centroid to any vertex is given by \( \frac{2}{3} \) of the median. ### Step 2: Calculate the Length of the Median The length of the median (AD) in an equilateral triangle can be calculated using the formula: \[ AD = \frac{\sqrt{3}}{2} \times \text{side} \] For a side of 9 cm: \[ AD = \frac{\sqrt{3}}{2} \times 9 = \frac{9\sqrt{3}}{2} \text{ cm} \] ### Step 3: Calculate the Distance from the Centroid to a Side The distance (OD) from the centroid to a side of the triangle (which is perpendicular to that side) is: \[ OD = \frac{1}{3} \times AD = \frac{1}{3} \times \frac{9\sqrt{3}}{2} = \frac{3\sqrt{3}}{2} \text{ cm} = \frac{3\sqrt{3}}{200} \text{ m} \] ### Step 4: Calculate the Magnetic Field Due to One Side Using the formula for the magnetic field due to a long straight conductor: \[ B = \frac{\mu_0 I}{4\pi r} \left( \sin \theta_1 + \sin \theta_2 \right) \] where: - \( \mu_0 = 4\pi \times 10^{-7} \, \text{T m/A} \) - \( I = 2 \, \text{A} \) - \( r = OD \) - \( \theta_1 = \theta_2 = 60^\circ \) (since the angles are equal in an equilateral triangle) Calculating \( \sin 60^\circ \): \[ \sin 60^\circ = \frac{\sqrt{3}}{2} \] Thus, \[ B_1 = \frac{\mu_0 I}{4\pi \left(\frac{3\sqrt{3}}{200}\right)} \left( \frac{\sqrt{3}}{2} + \frac{\sqrt{3}}{2} \right) = \frac{\mu_0 I}{4\pi r} \cdot \sqrt{3} \] ### Step 5: Calculate the Total Magnetic Field Since there are three sides contributing equally to the magnetic field at the centroid: \[ B_{total} = 3B_1 = 3 \left( \frac{\mu_0 I}{4\pi r} \cdot \sqrt{3} \right) \] ### Step 6: Substitute the Values Substituting the values into the equation: \[ B_{total} = 3 \left( \frac{4\pi \times 10^{-7} \times 2}{4\pi \times \frac{3\sqrt{3}}{200}} \cdot \sqrt{3} \right) \] Simplifying this gives: \[ B_{total} = 3 \left( \frac{2 \times 200 \times 10^{-7}}{3\sqrt{3}} \cdot \sqrt{3} \right) = 3 \left( \frac{400 \times 10^{-7}}{3} \right) = 4 \times 10^{-6} \text{ T} \] ### Step 7: Final Calculation Thus, the magnetic field at the centroid of the triangle is: \[ B = \frac{4}{3} \times 10^{-6} \text{ T} \approx 1.33 \times 10^{-6} \text{ T} \] ### Conclusion The magnetic field at the centroid of the equilateral triangle is approximately \( 1.33 \times 10^{-6} \text{ T} \). ---
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