Calculate Magnetic Force per Unit Length: The force per unit length \( \frac{F}{\ell} \) on a current-carrying conductor in a magnetic field is given by:
\[ \frac{F}{\ell} = i B \sin \theta \]
where:
\( i = \sqrt{2} \, \text{A} \) (current in the conductor)
\( B = 3.5 \times 10^{-5} \, \text{T} \) (magnetic field)
\( \theta = 45^\circ \) (angle between current direction and magnetic field)
Substitute Values: Using \( \sin 45^\circ = \frac{1}{\sqrt{2}} \):
\[ \frac{F}{\ell} = (\sqrt{2}) \times (3.5 \times 10^{-5}) \times \frac{1}{\sqrt{2}} = 35 \times 10^{-6} \, \text{N/m} \]
Conclusion: The force per unit length experienced by the conductor is:
\[ 35 \times 10^{-6} \, \text{N/m} \]
Group-I | Group-II | ||
P | Magnetic | 1 | Chargeability |
Q | Gravity | 2 | Electrical conductivity |
R | Magnetotelluric | 3 | Susceptibility |
S | Induced Polarization | 4 | Density |
Let a line passing through the point $ (4,1,0) $ intersect the line $ L_1: \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} $ at the point $ A(\alpha, \beta, \gamma) $ and the line $ L_2: x - 6 = y = -z + 4 $ at the point $ B(a, b, c) $. Then $ \begin{vmatrix} 1 & 0 & 1 \\ \alpha & \beta & \gamma \\ a & b & c \end{vmatrix} \text{ is equal to} $
Resonance in X$_2$Y can be represented as
The enthalpy of formation of X$_2$Y is 80 kJ mol$^{-1}$, and the magnitude of resonance energy of X$_2$Y is: