An infinitely long wire has uniform linear charge density . The net flux through a Gaussian cube of side length , if the wire passes through any two corners of the cube, that are maximally displaced from each other, would be , where is:
- A
- B
- C
- D
An infinitely long wire has uniform linear charge density . The net flux through a Gaussian cube of side length , if the wire passes through any two corners of the cube, that are maximally displaced from each other, would be , where is:
Correct answer:A
Standard Method
Given: An infinitely long wire has linear charge density . The cube has side length and the wire passes through two maximally displaced corners, so it lies along the body diagonal of the cube.
Find: The net electric flux through the cube.
Using Gauss's law,
The length of wire inside the cube is the body diagonal. For a cube of side , body diagonal is . Here , so
Therefore, enclosed charge is
Now,
Since , the flux matches .
Therefore, the correct option is A.
Why the wire length inside the cube is the body diagonal
Given: The wire passes through two corners of the cube that are maximally displaced from each other.
Find: The segment length of the wire enclosed by the cube.
The two maximally displaced corners of a cube are opposite vertices. The straight line joining them is the body diagonal.
If the side of the cube is , then the body diagonal is
Substituting ,
This is the wire length enclosed inside the cube. Then Gauss's law gives the same result:
Hence, the correct option is A.
Taking the wire length inside the cube as the side length is wrong because the wire passes through opposite corners, so the enclosed segment is the body diagonal, not an edge. Use .
Using directly is inappropriate here because the electric field is not uniform over the cube faces in a simple way. Use Gauss's law in the form .
Forgetting unit conversion leads to an incorrect enclosed charge. Convert to before multiplying by in .
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