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A straight section PQ of a circuit lies ...

A straight section PQ of a circuit lies along the x-axis from `x=-(a)/(2)` to `x=(a)/(2)` and carries a steady current i. The magnetic field due to the section PQ at a point x =+a will be

A

proportional to a

B

proportional to `a^(2)`

C

proportional to 1/a

D

zero

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The correct Answer is:
To solve the problem of finding the magnetic field due to a straight section PQ of a circuit at a point x = +a, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Configuration**: - The straight section PQ lies along the x-axis from \( x = -\frac{a}{2} \) to \( x = \frac{a}{2} \). - The point where we need to find the magnetic field is at \( x = a \). 2. **Using Biot-Savart Law**: - The Biot-Savart Law states that the magnetic field \( \mathbf{B} \) at a point due to a current-carrying conductor is given by: \[ d\mathbf{B} = \frac{\mu_0}{4\pi} \frac{I \, d\mathbf{l} \times \mathbf{r}}{r^3} \] - Here, \( I \) is the current, \( d\mathbf{l} \) is the current element, and \( \mathbf{r} \) is the position vector from the current element to the point where the field is being calculated. 3. **Identifying the Geometry**: - For the straight section PQ, we can consider a small current element \( d\mathbf{l} \) at a position \( x \) (where \( -\frac{a}{2} \leq x \leq \frac{a}{2} \)). - The position vector \( \mathbf{r} \) from the current element to the point \( x = a \) is \( \mathbf{r} = a - x \). 4. **Calculating the Angle**: - The angle \( \theta \) between the current element \( d\mathbf{l} \) and the vector \( \mathbf{r} \) is crucial for applying the Biot-Savart Law. - Since the current flows along the x-axis and the point is also on the x-axis, the angle \( \theta \) between \( d\mathbf{l} \) and \( \mathbf{r} \) is \( 0^\circ \). 5. **Evaluating the Magnetic Field**: - Since \( \sin(0^\circ) = 0 \), the contribution to the magnetic field from each current element \( d\mathbf{l} \) becomes zero: \[ d\mathbf{B} = \frac{\mu_0}{4\pi} \frac{I \, d\mathbf{l} \times \mathbf{r}}{r^3} = 0 \] - Therefore, the total magnetic field \( \mathbf{B} \) at point \( x = a \) is also zero. 6. **Conclusion**: - The magnetic field due to the straight section PQ at point \( x = a \) is: \[ \mathbf{B} = 0 \] ### Final Answer: The magnetic field at point \( x = a \) is \( 0 \). Therefore, the correct option is option 4.
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