Step 1: Recall the formula for magnetic field due to a straight current-carrying wire.
For a straight wire of finite length, the magnetic field at a point at perpendicular distance \( r \) from the wire is given by:
\[
B = \frac{\mu_0 I}{4\pi r} (\sin\theta_1 + \sin\theta_2)
\]
where \( \theta_1 \) and \( \theta_2 \) are the angles subtended by the wire at the point.
Step 2: For a point near the center of the wire.
When the point is opposite the center of the wire (perpendicular bisector), the angles are equal and maximum for a given distance.
Step 3: Analyze points X, Y, Z.
- Point Y is located directly above the center of wire AB (perpendicular bisector).
- Points X and Z are located above the ends of the wire (near A and B respectively).
- All three points are at the same perpendicular distance from the wire (same vertical height).
Step 4: Compare the angles.
- For point Y (center): The wire subtends maximum angles \( \theta_1 \) and \( \theta_2 \) (almost 90° each if wire is long).
- For points X and Z (near ends): The angles subtended are smaller because the point is not symmetrically placed with respect to the wire.
Step 5: Mathematical comparison.
For a wire of length \( L \), at perpendicular distance \( d \):
- At center: \( \sin\theta_1 + \sin\theta_2 = \frac{2 \times (L/2)}{\sqrt{(L/2)^2 + d^2}} = \frac{L}{\sqrt{(L/2)^2 + d^2}} \)
- At end: \( \sin\theta_1 + \sin\theta_2 = 0 + \frac{L}{\sqrt{L^2 + d^2}} = \frac{L}{\sqrt{L^2 + d^2}} \)
Since \( \sqrt{(L/2)^2 + d^2}<\sqrt{L^2 + d^2} \), the value at center is larger.
Step 6: Conclusion.
The magnetic field strength will be maximum at point Y because:
- It lies on the perpendicular bisector of the wire where the angles subtended by the wire are maximum.
- For the same perpendicular distance, the field is strongest at points opposite the center of the wire.
Step 7: Final answer.
The magnetic field strength will be maximum at point Y because it lies on the perpendicular bisector of the wire where the angles subtended by the wire are maximum.