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A long conducting wire of radius 1 cm carrying current of 1 A placed with its axis coinciding with X-axis. Find the magnetic field at point having coordinates `(0.5 cm, 0.5 cm )` .

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To find the magnetic field at the point (0.5 cm, 0.5 cm) due to a long conducting wire carrying a current of 1 A, we can use Ampere's Circuital Law. Let's go through the solution step by step. ### Step 1: Understand the Geometry The wire is a long straight conductor with its axis along the x-axis. The radius of the wire is 1 cm. The point where we need to find the magnetic field has coordinates (0.5 cm, 0.5 cm), which means it is located in the xy-plane. **Hint:** Visualize the wire and the point in a coordinate system to understand their positions relative to each other. ### Step 2: Determine the Distance from the Wire The point (0.5 cm, 0.5 cm) is at a distance from the wire. The distance \( r \) from the center of the wire to the point can be calculated using the Pythagorean theorem: \[ r = \sqrt{(0.5)^2 + (0.5)^2} = \sqrt{0.25 + 0.25} = \sqrt{0.5} \text{ cm} = 0.707 \text{ cm} \] **Hint:** Use the Pythagorean theorem to find the distance from the wire to the point. ### Step 3: Apply Ampere's Circuital Law According to Ampere's Circuital Law: \[ \oint \mathbf{B} \cdot d\mathbf{L} = \mu_0 I_{\text{enclosed}} \] For a circular path around the wire, the magnetic field \( B \) is constant along the path, so we can simplify the left side: \[ B \cdot (2\pi r) = \mu_0 I_{\text{enclosed}} \] **Hint:** Remember that \( I_{\text{enclosed}} \) is the current enclosed by the path. For a point outside the wire, the enclosed current is the total current flowing through the wire. ### Step 4: Calculate the Enclosed Current Since the point is outside the wire, the enclosed current \( I_{\text{enclosed}} \) is simply the total current flowing through the wire, which is given as 1 A. **Hint:** Identify that the current flowing through the wire is the same as the enclosed current when the point is outside the wire. ### Step 5: Substitute Values into the Equation Now we can substitute the values into the equation: \[ B \cdot (2\pi \cdot 0.707 \times 10^{-2}) = \mu_0 \cdot 1 \] Where \( \mu_0 = 4\pi \times 10^{-7} \, \text{T m/A} \). **Hint:** Make sure to convert all units to SI units for consistency. ### Step 6: Solve for B Rearranging the equation gives: \[ B = \frac{\mu_0 \cdot 1}{2\pi \cdot 0.707 \times 10^{-2}} \] Substituting the value of \( \mu_0 \): \[ B = \frac{4\pi \times 10^{-7}}{2\pi \cdot 0.707 \times 10^{-2}} = \frac{2 \times 10^{-7}}{0.707 \times 10^{-2}} = \frac{2 \times 10^{-5}}{0.707} \approx 2.83 \times 10^{-5} \, \text{T} \] **Hint:** When simplifying, ensure to keep track of the powers of ten and the constants. ### Final Answer The magnetic field at the point (0.5 cm, 0.5 cm) is approximately \( 2.83 \times 10^{-5} \, \text{T} \).
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