(II) Two long wires are oriented so that they are perpendicular to each other. At their closest, they are 20.0 cm apart (Fig. 28–42). What is the magnitude of the magnetic field at a point midway between them if the top one carries a current of 18.0 A and the bottom one carries 12.0 A?
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29. Sources of Magnetic Field
Magnetic Field Produced by Straight Currents
Problem 43
Textbook Question
(II) Consider a straight section of wire of length d, as in Fig. 28–51, which carries a current I. (a) Show that the magnetic field at a point P a distance 𝑅 from the wire along its perpendicular bisector is
(b) Show that this is consistent with Example 28–10 for an infinite wire.


1
Step 1: Begin by understanding the problem. Part (a) asks us to derive the magnetic field at a point P a distance R from the wire along its perpendicular bisector. Part (b) asks us to verify that the result is consistent with the magnetic field of an infinite wire. We'll use the Biot-Savart law for part (a) and compare the result to the formula for an infinite wire in part (b).
Step 2: For part (a), apply the Biot-Savart law, which states that the magnetic field d𝐵 due to a small segment of current-carrying wire is given by: . Here, μ₀ is the permeability of free space, I is the current, dl is the length element of the wire, θ is the angle between dl and the vector pointing to the observation point, and r is the distance from dl to the observation point.
Step 3: Consider the geometry of the problem. The wire is of finite length d, and the point P is located at a distance R from the wire along its perpendicular bisector. Symmetry simplifies the calculation: the contributions to the magnetic field from opposite sides of the wire will add up in the same direction. Use trigonometry to express sinθ and r in terms of R, d, and the position along the wire.
Step 4: Integrate the Biot-Savart law over the length of the wire from -d/2 to +d/2. The integral will involve terms like , which arise from the geometry of the problem. After performing the integration, simplify the result to obtain the magnetic field at point P: .
Step 5: For part (b), compare the derived formula to the magnetic field of an infinite wire, which is given by . As the length d approaches infinity, the term simplifies to 1, and the derived formula reduces to the infinite wire formula, confirming consistency.

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Key Concepts
Here are the essential concepts you must grasp in order to answer the question correctly.
Magnetic Field Due to a Current-Carrying Wire
The magnetic field generated by a straight current-carrying wire can be calculated using Ampère's Law. The magnetic field (B) at a distance (R) from the wire is directly proportional to the current (I) flowing through the wire and inversely proportional to the distance from the wire. This relationship is crucial for understanding how the magnetic field behaves around conductors.
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Magnetic Force on Current-Carrying Wire
Biot-Savart Law
The Biot-Savart Law provides a method to calculate the magnetic field produced at a point in space by a small segment of current-carrying wire. It states that the magnetic field (dB) at a point is proportional to the current (I), the length of the wire segment (dl), and the sine of the angle between the wire segment and the line connecting the segment to the point, divided by the square of the distance from the segment to the point.
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Biot-Savart Law with Calculus
Limit of Finite Wire to Infinite Wire
When analyzing the magnetic field of a finite wire, it is important to understand how it approaches the behavior of an infinite wire as the length of the wire increases. The magnetic field of an infinite wire is uniform and can be derived from the finite wire's magnetic field by taking the limit as the length approaches infinity, simplifying calculations and providing a clearer understanding of magnetic field behavior in practical applications.
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Magnetic Field due to Finite Wire
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