\(u=−MBcosθ\)
\(W=Δu\)
\(W=−MBcos180^0(−mBcos0^0)\)
\(W=2MB\)
\(W=2×5×0.4\)
\(W=4J\)
Therefore, the correct answer is (A): 4J
\(u=−MBcosθ\)
\(W=Δu\)
\(W=−MBcos180^0(−mBcos0^0)\)
\(W=2MB\)
\(W=2×5×0.4\)
\(W=4J\)
Therefore, the correct answer is (A): 4J
List I (Material) | List II (Subsceptibility(χ)) | ||
A. | Diamagnetic | I. | χ = 0 |
B. | Ferromagnetic | II. | 0 > χ ≥ –1 |
C. | Paramagnetic | III. | χ >> 1 |
D. | Non-magnetic | IV. | 0 < χ < ε (a small positive number) |
Moving charges generate an electric field and the rate of flow of charge is known as current. This is the basic concept in Electrostatics. Another important concept related to moving electric charges is the magnetic effect of current. Magnetism is caused by the current.
Region in space around a magnet where the Magnet has its Magnetic effect is called the Magnetic field of the Magnet. Let us suppose that there is a point charge q (moving with a velocity v and, located at r at a given time t) in presence of both the electric field E (r) and the magnetic field B (r). The force on an electric charge q due to both of them can be written as,
F = q [ E (r) + v × B (r)] ≡ EElectric +Fmagnetic
This force was based on the extensive experiments of Ampere and others. It is called the Lorentz force.