The gas is contained in a closed vessel, so the volume remains constant. This is an isochoric process. For an ideal gas at constant volume, the pressure is directly proportional to the temperature (in Kelvin): \[ P \propto T \implies \frac{P}{T} = \text{constant} \implies \frac{\Delta P}{\Delta T} = \frac{P}{T} \] Let the initial pressure be \( P \) and the initial temperature be \( T \) (in Kelvin).
The pressure increases by 0.4%, so the change in pressure \( \Delta P = 0.4% \text{ of } P = \frac{0.4}{100} P = 0.004 P \). The temperature is increased by \( 1^\circ \text{C} \), which is equal to \( 1 \, \text{K} \) change in Kelvin scale, so \( \Delta T = 1 \, \text{K} \).
Substituting these values into the equation: \[ \frac{0.004 P}{1} = \frac{P}{T} \] \[ 0.004 = \frac{1}{T} \] \[ T = \frac{1}{0.004} = \frac{1000}{4} = 250 \, \text{K} \] The initial temperature of the gas is \( 250 \, \text{K} \).
To convert this to Celsius, we use \( T(^\circ \text{C}) = T(K) - 273.15 \): \[ T(^\circ \text{C}) = 250 - 273.15 = -23.15^\circ \text{C} \] However, the options are given in Celsius and Kelvin, and \( 250 \, \text{K} \) is one of the options.
Match List - I with List - II.
Consider the following statements:
(A) Availability is generally conserved.
(B) Availability can neither be negative nor positive.
(C) Availability is the maximum theoretical work obtainable.
(D) Availability can be destroyed in irreversibility's.
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: