\( [B] = [e]^\alpha [m_e]^\beta [h]^\gamma [K]^\delta \)
\( [B] = MT^{-2} \)
\( [e] = I T \)
\( [h] = ML^2 T^{-1} \)
\( [K] = ML^3 T^{-4} I^{-2} \)
Now, equating the dimensions:
\( MT^{-2} = [IT]^\alpha [M]^\beta \)
\( [ML^2 T^{-1}]^\gamma [ML^3 T^{-4} I^{-2}]^\delta \)
This results in the following system of equations:
\( 1 = \beta + \gamma + \delta \) (1)
\( -2 = \alpha - \gamma - 4\delta \) (2)
\( -1 = \alpha - 2\delta \) (3)
\( 0 = 2\gamma + 3\delta \) (4)
Solving equations (1), (2), (3), and (4), we get:
\( \alpha = 3 \)
\( \gamma = -3 \)
\( \delta = 2 \)
\( \beta = 2 \)
Finally, \( \alpha + \beta + \gamma + \delta = 4 \)
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
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.