Total enthalpy change for freezing of 1 ~mol$1 \mathrm{~mol}$ of water at 10° C$10^{\circ} \mathrm{C}$ to ice at -10° C$-10^{\circ} \mathrm{C}$ is
(Given: ΔfusH = x$\Delta_{\mathrm{fus}}\mathrm{H} = \mathrm{x}$ kJ/mol, Cₚ[H₂O( )] = y J mol⁻¹ K⁻¹$\mathrm{C}_{\mathrm{p}}[\mathrm{H}_2\mathrm{O}(\ell)] = \mathrm{y}\text{ J mol}^{-1}\text{ K}^{-1}$, Cₚ[H₂O(s)] = z J mol⁻¹ K⁻¹$\mathrm{C}_{\mathrm{p}}[\mathrm{H}_2\mathrm{O}(\text{s})] = \mathrm{z}\text{ J mol}^{-1}\text{ K}^{-1}$)
Freezing is an exothermic process, so all three steps (cooling water, freezing, and cooling ice) must carry a negative sign. Factoring out -10$-10$ cleanly yields the expression -10(100x+y+z)$-10(100x+y+z)$.
20.0~dm³$20.0~\mathrm{dm}^{3}$ of an ideal gas 'X' at 600~K$600\mathrm{~K}$ and 0.5~MPa$0.5\mathrm{~MPa}$ undergoes isothermal reversible expansion until pressure of the gas is 0.2~MPa$0.2\mathrm{~MPa}$. Which of the following option is correct?
(Given: ~2=0.3010$\log~2=0.3010$ and ~5=0.6989$\log~5=0.6989$)
wᵢₛₒ = -nRT ln((P₁)/(P₂)) = -P₁ V₁ ln((P₁)/(P₂))$$w_{\text{iso}} = -nRT \ln\left(\frac{P_1}{P_2}\right) = -P_1 V_1 \ln\left(\frac{P_1}{P_2}\right)$$ \n Δ U = 0 and Δ H = 0 (For isothermal process)$$\Delta U = 0 \quad \text{and} \quad \Delta H = 0 \quad \text{(For isothermal process)}$$
Core Logic
For an isothermal reversible process involving an ideal gas, the change in internal energy (Δ U$\Delta U$) and change in enthalpy (Δ H$\Delta H$) are zero. By First Law of Thermodynamics, q = -w$q = -w$.
Isothermal expansion of an ideal gas always yields w < 0$w < 0$, q > 0$q > 0$, and Δ U = Δ H = 0$\Delta U = \Delta H = 0$. Matching signs instantly eliminates non-conforming options.
Comparing this with equation of straight line y = mx + c$y = mx + c$ where y = ₁₀K$y = \log_{10}K$ and x = (1)/(T)$x = \frac{1}{T}$:
Slope (m$m$) = - Δ H°2.303R$= -\frac{\Delta H^{\circ}}{2.303R}$
Intercept (c$c$) = Δ S°2.303R$= \frac{\Delta S^{\circ}}{2.303R}$
Step 1: Final Conclusion
The intercept is Δ S°2.303R$\frac{\Delta S^{\circ}}{2.303R}$ and the slope is - Δ H°2.303R$-\frac{\Delta H^{\circ}}{2.303R}$.
Pattern Recognition
Standard Van't Hoff thermodynamic plot derivation. Always remember to carry the negative sign from Δ G$\Delta G$ to the Enthalpy term.
Chapter Mix
Class 11 Chemistry: Thermodynamics
Class 11 Chemistry: Equilibrium
Q38jee_main_2025_02_april_eveningThermodynamic Work and Reversible Processes
Arrange the following in order of magnitude of work done by the system / on the system at constant temperature :
(a) |wreversible|$|\mathrm{w}_{\mathrm{reversible}}|$ for expansion in infinite stage.
(b) |wirreversible|$|\mathrm{w}_{\mathrm{irreversible}}|$ for expansion in single stage.
(c) |wreversible|$|\mathrm{w}_{\mathrm{reversible}}|$ for compression in infinite stage.
(d) |wirreversible|$|\mathrm{w}_{\mathrm{irreversible}}|$ for compression in single stage.
Choose the correct answer from the options given below:
A.a > b > c > d$a > b > c > d$
B.d > c = a > b$\mathrm{d} > \mathrm{c} = \mathrm{a} > \mathrm{b}$
Reversible Path: Since a reversible compression path retraces the exact coordinates of the reversible expansion path, the magnitudes of work are equal:
|wrev, expansion| = |wrev, compression| a = c$$|w_{\text{rev, expansion}}| = |w_{\text{rev, compression}}| \implies a = c$$
P-V indicator diagrams comparing reversible and irreversible expansion/compression
Isothermal Expansion: Reversible work magnitude is the maximum possible work. Hence, for expansion:
|wrev, expansion| > |wirrev, expansion| a > b$$|w_{\text{rev, expansion}}| > |w_{\text{irrev, expansion}}| \implies a > b$$
P-V indicator diagrams comparing reversible and irreversible expansion/compression
Isothermal Compression: Irreversible compression requires more work than reversible compression because of sudden pressure adjustments against the surroundings:
|wirrev, compression| > |wrev, compression| d > c$$|w_{\text{irrev, compression}}| > |w_{\text{rev, compression}}| \implies d > c$$
P-V indicator diagrams comparing reversible and irreversible expansion/compressionP-V indicator diagrams comparing reversible and irreversible expansion/compression
Step 1: Combine the inequalities
Combining the results:
We have a = c$a = c$
We have d > c$d > c$
We have a > b$a > b$
This leads to the strict inequality sequence:
d > c = a > b$d > c = a > b$
Pattern Recognition
Thermodynamics Principle: Reversible expansion is the most efficient (gives maximum work magnitude), whereas reversible compression is the most efficient (requires minimum work magnitude). Single-stage irreversible compression is always the least efficient, demanding the absolute highest work input.
Chapter Mix
Class 11 Chemistry: Chemical Thermodynamics
Qjee_main_2025_02_april_morningIdeal Gas Free Expansion
Two vessels A and B are connected via stopcock. The vessel A is filled with a gas at a certain pressure. The entire assembly is immersed in water and is allowed to come to thermal equilibrium with water. After opening the stopcock the gas from vessel A expands into vessel B and no change in temperature is observed in the thermometer. Which of the following statement is true?
The diagram displays a water bath calorimeter surrounding two interconnected glass flasks via a valve setup to demonstrate thermal expansion behavior.
A.(1) dw ≠ 0$(1)\ \mathrm{dw} \neq 0$
B.(2) dq ≠ 0$(2)\ \mathrm{dq} \neq 0$
C.(3) dU ≠ 0$(3)\ \mathrm{dU} \neq 0$
D.(4) The pressure in the vessel B before opening the stopcock is zero.$(4)\ \text{The pressure in the vessel B before opening the stopcock is zero.}$
Solution
Related Formula
First Law of Thermodynamics expression:
dU = dq + dw$$\mathrm{dU = dq + dw}$$
Core Logic
The system parameters show an isothermal transformation layout with zero overall heat transfer step:
No change in temperature signifies dT = 0$\mathrm{dT} = 0$, hence internal energy change for an ideal gas satisfies:
dU = nCvdT = 0$$\mathrm{dU} = nC_v\mathrm{dT} = 0$$
Since it expands freely into an empty chamber (vessel B), external pressure Pₑₓₜ = 0$P_{\text{ext}} = 0$, meaning work done is:
Combining these parameters in the First Law gives dq = 0$\mathrm{dq} = 0$.
This classic situation of "free expansion" implies vessel B was completely evacuated initially.
Step 1: Statement Verification
Therefore, the pressure inside vessel B before opening the stopcock was precisely zero.
Pattern Recognition
Isothermal + expansion against no opposing force = Free Expansion. For free expansion of an ideal gas, always remember: w = 0$w = 0$, q = 0$q = 0$, and Δ U = 0$\Delta U = 0$ simultaneously.
Chapter Mix
Class 11 Chemistry: Chemical Thermodynamics
Q41jee_main_2025_03_april_eveningLatent Heat and Phase Equilibrium
Given below are two statements:
Statement I: When a system containing ice in equilibrium with water (liquid) is heated, heat is absorbed by the system and there is no change in the temperature of the system until whole ice gets melted.
Statement II: At melting point of ice, there is absorption of heat in order to overcome intermolecular forces of attraction within the molecules of water in ice and kinetic energy of molecules is not increased at melting point.
In the light of the above statements, choose the correct answer from the options given below:
A. Statement I is true but Statement II is false
B. Both Statement I and Statement II are false
C. Both Statement I and Statement II are true
D. Statement I is false but Statement II is true
Solution
Related Formula
During phase transition, latent heat of fusion (Lf$L_f$) is absorbed:
Q = m Lf$Q = m L_f$
Temperature remains constant because the average kinetic energy of the molecules does not change; instead, potential energy changes during phase transition:
Temperature T ∝ Average Kinetic Energy of molecules$$\text{Temperature } T \propto \text{Average Kinetic Energy of molecules}$$
Core Logic
Statement I Analysis:
During a phase transition (such as ice melting at 0°C$0^{\circ}\mathrm{C}$), any added heat is utilized as latent heat of fusion. The system remains at a constant temperature of 0°C$0^{\circ}\mathrm{C}$ as long as both solid and liquid phases coexist in equilibrium. Thus, Statement I is True.
Step 1: Analyze Statement II
Statement II explains why this happens: The thermal energy is spent entirely to break down the highly ordered crystalline hydrogen-bonded lattice of ice into liquid water. It does not increase the translational kinetic energy of the molecules. Since kinetic energy is constant, temperature remains constant. Thus, Statement II is True.
Step 2: Conclusion
Therefore, both Statement I and Statement II are True, matching Option (3).
Pattern Recognition
For any phase transition (melting, boiling, sublimation): Temperature stays flat. The added energy goes entirely into latent heat (potential energy change to overcome intermolecular forces), meaning average kinetic energy is constant.
Chapter Mix
Class 11 Chemistry: Thermodynamics
Class 11 Physics: Thermal Properties of Matter
More Chemical Thermodynamics Questions — jee_main_2025_07_april_morning
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.