The emf (\( \varepsilon \)) induced in an inductor is related to the rate of change of current and self-inductance (\( L \)) by the formula:
\[ |\varepsilon| = L \frac{dI}{dt}. \]
Step 1: Determine the rate of change of current
The given current is:
\[ I = 3t + 8. \]
Differentiate \( I \) with respect to \( t \):
\[ \frac{dI}{dt} = 3 \, \text{A/s}. \]
Step 2: Substitute the given values
The magnitude of induced emf is \( |\varepsilon| = 12 \, \text{mV} = 12 \times 10^{-3} \, \text{V} \). Substituting into the formula:
\[ 12 \times 10^{-3} = L \cdot 3. \]
Step 3: Solve for \( L \)
Rearrange to find \( L \):
\[ L = \frac{12 \times 10^{-3}}{3} = 4 \times 10^{-3} \, \text{H}. \]
Convert to millihenries:
\[ L = 4 \, \text{mH}. \]
Thus, the self-inductance of the inductor is \( L = 4 \, \text{mH} \).
As shown in the diagram, an electron enters perpendicularly into a magnetic field. Using Fleming’s Left-Hand Rule, determine the direction of the force experienced by the electron.
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).