Which of the following conditions regarding a chemical process ensures its spontaneity at all temperature? (a) \(\Delta H>0, \Delta G<0\) (b) \(\Delta H<0, \Delta S>0\) (c) \(\Delta H<0, \Delta S<0\) (d) \(\Delta H>0, \Delta S<0\)

Short Answer

Expert verified
The condition that ensures spontaneity at all temperatures is (b) \(\Delta H<0, \Delta S>0\

Step by step solution

01

Understanding Spontaneity

A chemical process is spontaneous if it can occur without being driven by some external force. To determine the spontaneity, we consider the Gibbs free energy change \(\Delta G\), which is defined by the equation \(\Delta G = \Delta H - T\Delta S\), where \(\Delta H\) is the change in enthalpy, \(T\) is the temperature in Kelvin, and \(\Delta S\) is the change in entropy.
02

Gibbs Free Energy and Temperature Dependency

The sign of \(\Delta G\) determines spontaneity. For a process to be spontaneous at all temperatures, \(\Delta G\) should always be negative, regardless of the value of \(T\). This means the signs of \(\Delta H\) and \(\Delta S\) must be such that \(\Delta G\) remains negative even as \(T\) changes.
03

Evaluating the Given Options

Looking at the options given: (a) Does not ensure spontaneity at high temperatures because positive \(\Delta H\) might lead to a positive \(\Delta G\) at high \(T\). (b) Ensures spontaneity because a negative \(\Delta H\) and a positive \(\Delta S\) always yield a negative \(\Delta G\), regardless of \(T\). (c) and (d) will not ensure spontaneity at all temperatures because negative \(\Delta S\) could lead to \(\Delta G\) becoming positive at low temperature in (c) and at high temperature in (d).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Gibbs Free Energy
Gibbs free energy, represented by the symbol \( G \), is a measure of the maximum reversible work that may be performed by a thermodynamic system at a constant temperature and pressure. It is a pivotal concept in determining the spontaneity of chemical reactions. The equation that defines Gibbs free energy is \( \Delta G = \Delta H - T\Delta S \), where \( \Delta G \) is the change in Gibbs free energy, \( \Delta H \) is the change in enthalpy, \( T \) is the absolute temperature, and \( \Delta S \) is the change in entropy.

A negative value of \( \Delta G \) indicates that a process is spontaneous, which means it can occur without the input of external energy. Conversely, a positive \( \Delta G \) suggests that the process is non-spontaneous and requires energy to proceed. Importantly, a value of zero indicates a system in equilibrium, where the forward and reverse reactions occur at equal rates.
Enthalpy Change (\(\Delta H\))
Enthalpy change, denoted as \( \Delta H \), is the amount of heat absorbed or released by a system during a process at constant pressure. It is an extensive property and plays a crucial role in thermodynamics and chemistry, particularly in the study of heat transfer during chemical reactions.

When \( \Delta H \) is negative, the process is exothermic, meaning that heat is released into the surroundings; this is often associated with the formation of chemical bonds. On the other hand, a positive \( \Delta H \) indicates an endothermic process, in which the system absorbs heat and often involves breaking chemical bonds. The sign of \( \Delta H \) can also influence Gibbs free energy and the spontaneity of the reaction.
Entropy Change (\(\Delta S\))
Entropy, symbolized as \( S \), is a measure of the disorder or randomness in a system, and \( \Delta S \) signifies the change in entropy. In a chemical reaction, it reflects the degree to which energy is distributed among the possible motions and configurations of molecules.

An increase in entropy (\( \Delta S > 0 \) ) suggests more disorder; for instance, when a solid melts into a liquid. Conversely, a decrease in entropy (\( \Delta S < 0 \) ) represents a transition to a more ordered state, such as a gas condensing into a liquid. Entropy is also closely tied to the feasibility of a chemical process. Spontaneity at all temperatures requires both a negative change in enthalpy and a positive change in entropy.
Temperature Dependence in Chemical Reactions
The temperature of a system, commonly measured in Kelvin (\( K \)), fundamentally influences the rate and spontaneity of chemical reactions. Temperature serves as a critical factor in the Gibbs free energy equation, acting as a multiplier to the entropy change (\( T\Delta S \) ).

At higher temperatures, entropy plays a more significant role in determining \( \Delta G \), potentially shifting a non-spontaneous reaction (positive \( \Delta G \)) to a spontaneous one (negative \( \Delta G \)) if \( \Delta S \) is positive. Conversely, at low temperatures, the value of the enthalpy change (\( \Delta H \)) is more dominant. Understanding the temperature dependence is key to controlling reaction conditions in industrial and laboratory settings to ensure the desired outcome.

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Most popular questions from this chapter

Calculate standard entropy change in the reaction $$ \mathrm{Fe}_{2} \mathrm{O}_{3}(s)+3 \mathrm{H}_{2}(g) \longrightarrow 2 \mathrm{Fe}(s)+3 \mathrm{H}_{2} \mathrm{O}(l) $$ Given : \(S_{m}^{\circ}\left(\mathrm{Fe}_{2} \mathrm{O}_{3}, \mathrm{~S}\right)=87.4, S_{m}^{\circ}(\mathrm{Fe}, S)=27.3\) \(S_{m}^{\circ}\left(\mathrm{H}_{2}, g\right)=130.7, S_{m}^{\circ}\left(\mathrm{H}_{2} \mathrm{O}, l\right)=69.9 \mathrm{JK}^{-1} \mathrm{~mol}^{-1}\)

When one mole of an ideal gas is compressed to half of its initial volume and simultaneously heated to twice its initial temperature, the change in entropy of gas \((\Delta S)\) is : (a) \(C_{p, m} \ln 2\) (b) \(C_{v, m} \ln 2\) (c) \(R \ln 2\) (d) \(\left(C_{v, m}-R\right) \ln 2\)

10 mole of ideal gas expand isothermally and reversibly from a pressure of \(10 \mathrm{~atm}\) to \(1 \mathrm{~atm}\) at \(300 \mathrm{~K}\). What is the largest mass which can lifted through a height of 100 meter? (a) \(31842 \mathrm{~kg}\) (b) \(58.55 \mathrm{~kg}\) (c) \(342.58 \mathrm{~kg}\) (d) None of these

Calculate the final temperature of a monoatomic ideal gas that is compressed reversible and adiabatically from \(16 \mathrm{~L}\) to \(2 \mathrm{~L}\) at \(300 \mathrm{~K}\) : (a) \(600 \mathrm{~K}\) (b) \(1044.6 \mathrm{~K}\) (c) \(1200 \mathrm{~K}\) (d) \(2400 \mathrm{~K}\)

The heat of formation of \(\mathrm{NH}_{3}(g)\) is \(-46 \mathrm{~kJ} \mathrm{~mol}^{-1}\). The \(\Delta H\) (in \(\mathrm{kJ} \mathrm{mol}^{-1}\) ) of the reaction, \(2 \mathrm{NH}_{3}(g) \longrightarrow \mathrm{N}_{2}(g)+3 \mathrm{H}_{2}(g)\) is : (a) 46 (b) \(-46\) (c) 92 (d) \(-92\)

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