The equivalent resistance $R_\text{eq}$ of two resistors in parallel is given by:
\[ R_\text{eq} = \frac{10^4 R}{10^4 + R}. \]
Given: \[ E = 4 \, \text{V}, \quad I = 2 \, \text{mA}. \]
From Ohm's Law: \[ I = \frac{E}{R_\text{eq}}. \]
Substitute $R_\text{eq}$ into the equation:
\[ 2 \times 10^{-3} = \frac{4}{\frac{10^4 R}{10^4 + R}}. \]
Simplify: \[ 2 \times 10^{-3} = \frac{4(10^4 + R)}{10^4 R}. \]
Multiply through by $10^4 R$: \[ 2 \times 10^4 R = 4(10^4 + R). \]
Distribute and simplify: \[ 20R = 40000 + 4R. \]
Rearranging terms: \[ 16R = 40000. \]
Solve for $R$: \[ R = \frac{40000}{16} = 2500 \, \Omega. \]
Thus, the resistance $R$ is: \[ \boxed{2500 \, \Omega}. \]
Explanation: The equivalent resistance for two parallel resistors is determined by the formula $R_\text{eq} = \frac{10^4 R}{10^4 + R}$. By using the provided voltage and current values, Ohm's Law was applied to derive $R$. The algebraic simplifications lead to $R = 2500 \, \Omega$.
A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is:
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: