
- A40 A, perpendicular into the page
- B40 A, perpendicular out of the page
- C20 A, perpendicular into the page
- D40 A, perpendicular out of the page
View written solutionFree
Correct answer: C
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Interpret the geometry
Two identical infinitely long wires are bent at right angles.
- Wire 1 has horizontal part along the -axis and vertical part parallel to -axis.
- Wire 2 has horizontal part along the -axis and vertical part parallel to -axis.
- The point lies on the -axis such that
From the standard bent-wire arrangement, the two bends are symmetrically placed about , so the horizontal segments lie along the same line as .
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Field due to horizontal segments at
For any small current element on the horizontal parts or , the vector from the element to is along the same line as .
Hence,
So, horizontal segments contribute zero magnetic field at .
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Field due to each vertical semi-infinite segment
Each vertical part ( and ) is a semi-infinite straight wire at perpendicular distance from .
Magnetic field at distance due to a semi-infinite straight wire is
Therefore, field due to one vertical segment at is
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Net magnetic field at
By right-hand rule, the fields due to the two vertical segments are in the same perpendicular direction at , so they add.
Thus,
= \frac{\mu_0 I}{2\pi r}.$$ Given $$B_{\text{net}} = 10^{-4}\text{ T}.$$ So, $$10^{-4} = \frac{4\pi\times 10^{-7} \cdot I}{2\pi \cdot 0.04}.$$ -
Solve for
Simplify: or directly,
Better simplifying carefully:
= \frac{2\times10^{-7} I}{0.04} = 5\times10^{-6} I.$$ Hence, $$10^{-4} = 5\times10^{-6} I$$ $$I = \frac{10^{-4}}{5\times10^{-6}} = 20\text{ A}.$$ -
Direction of magnetic field
Using the right-hand rule for the current directions shown in the figure, the magnetic fields due to both vertical segments at are directed into the page. Hence the resultant field is also into the page.
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Match with options
- Current in each wire
- Direction of magnetic field at : perpendicular into the page
Therefore, the correct option is:
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