A very long straight conductor, carrying the steady current I₁, lies in the plane of a rectangular loop with N₂ turns. The straight long wire is at a distance a from the loop. 1₂ = 0 → Apply Ampere's law to derive the expression of the vector of magnetic field intensity (direction and magnitude) inside the loop, due to I₁, and draw the field intensity vector on the figure. y I1 ZO 12 a N₂ b X

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A very long straight conductor, carrying the steady current I₁, lies in the plane
of a rectangular loop with N₂ turns. The straight long wire is at a distance a
from the loop.
I₂ = 0 → Apply Ampere's law to derive the expression of the vector of magnetic
field intensity (direction and magnitude) inside the loop, due to I₁, and draw
the field intensity vector on the figure.
y
11
ZO
124
a
N₂
b
X
Transcribed Image Text:A very long straight conductor, carrying the steady current I₁, lies in the plane of a rectangular loop with N₂ turns. The straight long wire is at a distance a from the loop. I₂ = 0 → Apply Ampere's law to derive the expression of the vector of magnetic field intensity (direction and magnitude) inside the loop, due to I₁, and draw the field intensity vector on the figure. y 11 ZO 124 a N₂ b X
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