The Divinity of the Vedas, The Power of Knowledge — Vidaara
वेदों की दिव्यता, विद्या की शक्ति — विदारा
Conceived, Designed & Developed BySachin Sharma
An ideal gas undergoes a cyclic process $A \to B \to A$. Total $\Delta U$:
The work done in compressing a gas adiabatically from $V_1, P_1$ to $V_2, P_2$:
Carnot's theorem implies:
The change in internal energy when $1$ mole of monatomic ideal gas is heated from $300$ K to $400$ K:
The kinetic energy of $1$ mole of nitrogen at $T$ K:
The pressure of $2$ moles of an ideal gas at $300$ K in a container of $24.93$ L is:
The RMS speeds of O₂ and H₂ at same temperature are in ratio:
For an adiabatic process, the slope of $P-V$ curve compared to isothermal:
A heat engine receives $Q_1$ at $400$ K, rejects $Q_2$ at $300$ K. For Carnot, $Q_2/Q_1$:
The molar heat capacity at constant pressure ($C_P$) for a diatomic gas:
A Carnot engine operates between $T_1 = 600$ K and $T_2 = 300$ K. Its efficiency (in %):
The ratio of $\gamma$ for monatomic to that for diatomic gas, multiplied by $10$, is the integer:
The translational KE per molecule of an ideal gas at $300$ K, in units of $10^{-21}$ J (rounded):
Assertion (A): The internal energy of an ideal gas depends only on its temperature. Reason (R): There are no intermolecular forces in an ideal gas.
Assertion (A): A Carnot engine cannot have $100\%$ efficiency unless the cold reservoir is at $0$ K. Reason (R): Efficiency of Carnot engine is $1 - T_2/T_1$.
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