Question
Question: A single circular loop of wire with radius 0.02 m carries a current of 8.0 A. It is placed at the ce...
A single circular loop of wire with radius 0.02 m carries a current of 8.0 A. It is placed at the centre of a long solenoid that has length 0.65m, radius 0.080 m and 1300 turns. (Axis of circular loop coincide with axis of solenoid). Let 'i' be the current in solenoid.

If i=100 mA, the magnetic field at the center of coil can be zero.
If i = 44 mA, the magnetic field at the center of coil can be zero.
If i = 100 mA, the magnetic field at the center of coil can be 8π×10−5 T.
If i = 100 mA, the magnetic field at the center of coil can be 16π×10−5 T.
If i=100 mA, the magnetic field at the center of coil can be zero. If i = 100 mA, the magnetic field at the center of coil can be 16π×10−5 T.
Solution
The magnetic field at the center of the circular loop of radius Rc=0.02 m carrying current Ic=8.0 A is given by Bc=2Rcμ0Ic.
Bc=2×0.02 m4π×10−7 T m/A×8.0 A=0.0432π×10−7 T=800π×10−7 T=8π×10−5 T.
The number of turns per unit length of the solenoid is n=LN=0.65 m1300=2000 turns/m.
The magnetic field inside a long solenoid, at its center, is given by Bs=μ0ni, where i is the current in the solenoid.
Bs=(4π×10−7 T m/A)×(2000 m−1)×i=8π×10−4i T/A.
The circular loop is placed at the center of the solenoid with coincident axes. The magnetic field due to the loop and the solenoid at the center are along the common axis. The total magnetic field at the center is the vector sum of the two fields. The direction of the field due to the loop is fixed by the direction of Ic. The direction of the field due to the solenoid depends on the direction of i. The two fields can be in the same direction or opposite directions. The magnitude of the total magnetic field is ∣Bc±Bs∣.
Let's evaluate the given statements:
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Statement 1: If i=100 mA, the magnetic field at the center of coil can be zero. i=100 mA =0.1 A. Bs=8π×10−4 T/A×0.1 A=8π×10−5 T. Bc=8π×10−5 T. If the currents are directed such that the magnetic fields are in opposite directions, the total magnetic field magnitude is ∣Bc−Bs∣=∣8π×10−5−8π×10−5∣=0. So, the magnetic field at the center can be zero. Statement 1 is true.
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Statement 2: If i=44 mA, the magnetic field at the center of coil can be zero. i=44 mA =0.044 A. Bs=8π×10−4 T/A×0.044 A=3.52π×10−5 T. Bc=8π×10−5 T. For the total field to be zero, we need Bs=Bc. Since 3.52π×10−5=8π×10−5, the magnetic field at the center cannot be zero. Statement 2 is false.
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Statement 3: If i=100 mA, the magnetic field at the center of coil can be 8π×10−5 T. As calculated in Statement 1, when i=100 mA, Bs=8π×10−5 T and Bc=8π×10−5 T. The possible magnitudes of the total magnetic field are ∣Bc±Bs∣=∣8π×10−5±8π×10−5∣. This gives possible magnitudes 0 (when fields are opposite) and 16π×10−5 T (when fields are in the same direction). The value 8π×10−5 T is not a possible magnitude for the total field. Statement 3 is false.
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Statement 4: If i=100 mA, the magnetic field at the center of coil can be 16π×10−5 T. As calculated in Statement 3, when i=100 mA, Bs=8π×10−5 T and Bc=8π×10−5 T. If the currents are directed such that the magnetic fields are in the same direction, the total magnetic field magnitude is Bc+Bs=8π×10−5+8π×10−5=16π×10−5 T. So, the magnetic field at the center can be 16π×10−5 T. Statement 4 is true.
The correct statements are 1 and 4.