Mathematical Derivation
\[ \Lambda_m = \frac{K \times 1000}{C} \]
\[ 100 = \frac{K \times 1000}{0.0225} \]
\[ K = \frac{0.0225}{10} = \frac{1}{R} \times \frac{\ell}{A} \]
\[ \frac{\ell}{A} = \frac{0.0225}{10} \times 100 = 0.0225 \]
For lower concentration:
\[ \Lambda_m = \frac{K \times 1000}{C} \]
\[ 150 = \frac{K \times 1000}{0.01} \]
\[ K = \frac{0.15}{100} \]
\[ K = \frac{1}{R} \times \frac{\ell}{A} \]
\[ \frac{0.15}{100} = \frac{1}{R} \times 0.225 \]
\[ R = \frac{22.5}{0.15} = \frac{2250}{15} = 150\,\Omega \]
The left and right compartments of a thermally isolated container of length $L$ are separated by a thermally conducting, movable piston of area $A$. The left and right compartments are filled with $\frac{3}{2}$ and 1 moles of an ideal gas, respectively. In the left compartment the piston is attached by a spring with spring constant $k$ and natural length $\frac{2L}{5}$. In thermodynamic equilibrium, the piston is at a distance $\frac{L}{2}$ from the left and right edges of the container as shown in the figure. Under the above conditions, if the pressure in the right compartment is $P = \frac{kL}{A} \alpha$, then the value of $\alpha$ is ____
The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
The term independent of $ x $ in the expansion of $$ \left( \frac{x + 1}{x^{3/2} + 1 - \sqrt{x}} \cdot \frac{x + 1}{x - \sqrt{x}} \right)^{10} $$ for $ x>1 $ is: