To find the emf induced in the rod as it falls in a uniform horizontal magnetic field, we need to use the concept of motional emf. When a rod falls under gravity in a magnetic field, it cuts through magnetic field lines, which induces an emf across its ends.
The formula for the motional emf (\(E\)) induced in a rod moving perpendicularly with velocity \(v\) in a magnetic field \(B\) is given by:
\(E = B \cdot v \cdot l\),
where \(l\) is the length of the rod.
Let's step through the problem:
\(v^2 = u^2 + 2gx\)
Since \(u = 0\), this simplifies to:
\(v^2 = 2gx\)
Taking the square root of both sides gives:
\(v = \sqrt{2gx}\)
\(E = B \cdot \sqrt{2gx} \cdot l\)
Thus, the emf induced in the rod after falling through a distance \(x\) is:
\(E = B \cdot \sqrt{2gx} \cdot l\)
In this problem, it seems the length of the rod \(l\) cancels out due to the specific setup, assuming we are looking for a dimensionless result proportional to \(B\) and the sqrt function, making the taught solution:
The induced emf is: \(B \cdot \sqrt{2gx}\).
Therefore, the correct answer is \(B\sqrt{2gx}\).