Thermodynamics Fundamentals
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Questions and Answers

A scientist is studying a chemical reaction in a sealed, insulated container. Can the system exchange energy or matter with its surroundings? What type of system is this?

No, it cannot exchange energy or matter. This is an isolated system.

A researcher measures the temperature and pressure of a gas in a closed container. Are these properties considered extensive or intensive? Briefly explain why.

These are intensive properties because they do not depend on the amount of gas present in the container.

Consider two beakers, one containing 50 mL of water and the other containing 100 mL of water, both at the same temperature. Which property, volume or temperature, is an extensive property in this scenario? Explain.

Volume is an extensive property because it changes with the amount of water. The beaker with 100 mL of water has a larger volume.

A student is conducting an experiment where heat is released during a chemical reaction in a calorimeter. Is heat a state function or a path function? Explain your answer.

<p>Heat is a path function because the amount of heat exchanged depends on the specific process or path taken during the reaction.</p> Signup and view all the answers

Imagine a scenario where you have a balloon that can expand or contract. If you heat the balloon, causing it to expand, which macroscopic properties are most likely to change? Name two.

<p>Volume and potentially temperature. The volume will increase as the balloon expands, and the temperature may increase depending on the amount of heat.</p> Signup and view all the answers

A chemist investigates a reaction in a system that allows the transfer of energy but not matter. What type of system is the chemist working with, and what is an example of such a system?

<p>This is a closed system. An example would be a sealed container with a fixed amount of gas that can be heated or cooled.</p> Signup and view all the answers

Two different pathways are used to convert reactant A to product B. If the change in internal energy is measured to be the same for both pathways, what does this indicate about internal energy?

<p>This indicates that internal energy is a state function, as the change in its value is independent of the path taken.</p> Signup and view all the answers

How does increasing the amount of a substance in a system affect its extensive properties, and why is this distinction important in thermodynamic studies?

<p>Increasing the amount of a substance increases its extensive properties because these properties depend on the amount of matter. This distinction is important because it helps in scaling up or down processes and understanding the effects of quantity on system behavior.</p> Signup and view all the answers

Under what specific condition is the change in internal energy ($\Delta U$) of a system equal to the heat absorbed or released at constant volume ($q_v$)?

<p>When the volume is constant, meaning (\Delta V = 0).</p> Signup and view all the answers

How does the first law of thermodynamics relate the change in internal energy ($\Delta U$) to heat (q) and work (w)?

<p>The first law of thermodynamics states that (\Delta U = q + w), where q is the heat absorbed by the system and w is the work done on the system.</p> Signup and view all the answers

For an isothermal reversible process, what is the relationship between heat (q) and work (w) in terms of volume change?

<p>For an isothermal reversible process, (q = -w = 2.303nRT \log \frac{V_2}{V_1}), where (V_2) and (V_1) are the final and initial volumes, respectively.</p> Signup and view all the answers

What is the change in internal energy for a free expansion process and why?

<p>The change in internal energy is zero because no work is done since the external pressure is zero.</p> Signup and view all the answers

Differentiate between internal energy and enthalpy.

<p>Internal energy (U) comprises all energies within a system, while enthalpy (H) sums internal energy and pressure-volume energy, i.e., (H = U + PV).</p> Signup and view all the answers

In an adiabatic process, what condition applies to the heat transfer (q), and how does this simplify the first law of thermodynamics?

<p>In an adiabatic process, (q = 0). Therefore, the first law simplifies to (\Delta U = w), meaning the change in internal energy is solely due to work done.</p> Signup and view all the answers

What happens to the internal energy of system containing only solid/liquids? Explain why.

<p>The volume is constant, (\Delta V = 0 ). Therefore, (\Delta U = q).</p> Signup and view all the answers

What is free expansion? Is work done during free expansion?

<p>Free expansion is the expansion of gas into vacuum where external pressure is 0. No work is done.</p> Signup and view all the answers

Explain how Hess's Law allows for the calculation of enthalpy changes for reactions that are difficult or impossible to measure directly.

<p>Hess's Law states that the total enthalpy change for a reaction is the same whether it occurs in one step or multiple steps. This allows us to calculate the enthalpy change of a reaction by summing the enthalpy changes of a series of reactions that add up to the overall reaction.</p> Signup and view all the answers

How does the enthalpy of fusion relate to the intermolecular forces within a solid?

<p>The enthalpy of fusion is the energy required to overcome the intermolecular forces holding the solid together, allowing it to transition to the liquid phase. Stronger intermolecular forces result in a higher enthalpy of fusion.</p> Signup and view all the answers

Why is the standard enthalpy of combustion always a negative value?

<p>The standard enthalpy of combustion is always negative because combustion reactions are exothermic, meaning they release heat. The release of heat corresponds to a decrease in the enthalpy of the system.</p> Signup and view all the answers

What is a thermochemical equation, and what information does it convey beyond a standard chemical equation?

<p>A thermochemical equation is a balanced chemical equation that includes the enthalpy change ($\Delta rH0$) for the reaction. It specifies the physical states of all reactants and products and indicates whether heat is absorbed or released.</p> Signup and view all the answers

Describe how the enthalpy of vaporization differs from the enthalpy of sublimation at a molecular level.

<p>Enthalpy of vaporization involves a phase change from liquid to gas, requiring energy to overcome intermolecular forces in the liquid. Enthalpy of sublimation involves a direct phase change from solid to gas, overcoming stronger intermolecular forces in the solid state.</p> Signup and view all the answers

Explain why the physical states of reactants and products are important to specify in a thermochemical equation.

<p>The enthalpy change of a reaction is dependent on the physical states of the reactants and products (solid, liquid, gas) because the energy required to change phases (e.g., vaporization, fusion) contributes to the overall enthalpy change. Different physical states have different internal energies.</p> Signup and view all the answers

If a reaction occurs in two steps where $\Delta H_1$ is +50 kJ/mol and $\Delta H_2$ is -30 kJ/mol, what is the overall enthalpy change for the reaction, and is the reaction endothermic or exothermic?

<p>The overall enthalpy change is +20 kJ/mol (+50 kJ/mol - 30 kJ/mol). Since the overall $\Delta H$ is positive, the reaction is endothermic, meaning it absorbs heat from the surroundings.</p> Signup and view all the answers

How can you determine the enthalpy change for the reverse of a given reaction if you know the enthalpy change for the forward reaction?

<p>The enthalpy change for the reverse reaction is equal in magnitude but opposite in sign to the enthalpy change for the forward reaction. If the forward reaction has an enthalpy change of $\Delta H$, the reverse reaction will have an enthalpy change of -$\Delta H$.</p> Signup and view all the answers

Explain why a decrease in energy is not the sole criterion for spontaneity, providing an example to support your explanation.

<p>A decrease in energy cannot be the only criteria because some spontaneous processes, such as the melting of ice, involve the absorption of heat, which increases the energy of the system. These processes occur due to an increase in entropy that overcomes the energy increase.</p> Signup and view all the answers

How does the second law of thermodynamics define the spontaneity of a process in terms of entropy?

<p>The second law of thermodynamics states that for a spontaneous process, the total entropy of the universe (system plus surroundings) must increase.</p> Signup and view all the answers

Describe the relationship between entropy change and equilibrium in a system.

<p>At equilibrium, the entropy of the system is at its maximum, and the total entropy change (S Total) for the system and surroundings is zero.</p> Signup and view all the answers

Differentiate between a spontaneous and a non-spontaneous process, giving an example of each.

<p>A spontaneous process occurs without external intervention (e.g., the rusting of iron), while a non-spontaneous process requires continuous external energy input to proceed (e.g., electrolysis of water).</p> Signup and view all the answers

A system absorbs 500 J of heat reversibly at a temperature of 300 K. Calculate the change in entropy (S) for this process.

<p>$\Delta S = \frac{q_{rev}}{T} = \frac{500 \text{ J}}{300 \text{ K}} = 1.67 \text{ J/K}$</p> Signup and view all the answers

Explain how entropy generally changes during phase transitions (solid to liquid, liquid to gas) and why.

<p>Entropy increases during phase transitions from solid to liquid and liquid to gas because molecules gain more freedom of movement and occupy a larger volume, increasing the disorder or randomness of the system.</p> Signup and view all the answers

Is the mixing of gases considered a spontaneous process? Briefly justify your answer in terms of entropy change.

<p>Yes, the mixing of gases is a spontaneous process because it results in an increase in entropy as different gas molecules occupy a greater volume and become more disordered.</p> Signup and view all the answers

For the reaction $N_2(g) + 3H_2(g) \rightarrow 2NH_3(g)$ with $_rH^0 = -46.1 \text{ kJ/mol}$, is the reaction spontaneous at all temperatures? Explain your reasoning.

<p>It cannot be determined if the reaction is spontaneous at all temperatures based on only enthalpy. To determine the spontaneity, you would need to know the entropy change. If entropy is positive, it is spontaneous at high temperatures. If entropy is negative, it may be spontaneous at low temperatures. If the entropy change is zero, then temperature does not affect spontaneity.</p> Signup and view all the answers

Explain why $C_p$ is always greater than $C_v$ for an ideal gas. Relate your answer to the molecular level.

<p>At constant volume, all heat added goes into increasing the internal energy (kinetic energy) of the molecules, thus raising the temperature. At constant pressure, some of the added heat is used to do work against the surroundings as the gas expands, so less heat is available to raise the temperature.</p> Signup and view all the answers

A certain reaction has a positive $\Delta rH$. Explain what this indicates about the energy required for the reaction to occur and the stability of the products relative to the reactants.

<p>A positive $\Delta rH$ indicates that the reaction is endothermic, meaning it requires energy input to proceed. The products have higher enthalpy (energy) than the reactants, implying that the reactants are more stable than the products.</p> Signup and view all the answers

Consider a reaction where ΔH is negative. How does this information help you predict the effect of decreasing the temperature on the equilibrium constant (K) of the reaction?

<p>A negative ΔH means the reaction is exothermic. Decreasing the temperature will shift the equilibrium towards the products, increasing the equilibrium constant K. This is because the system will try to counteract the decrease in temperature by favoring the heat-releasing (exothermic) direction.</p> Signup and view all the answers

Explain how the third law of thermodynamics allows for the determination of absolute entropy values.

<p>The third law states that the entropy of a perfectly crystalline substance is zero at absolute zero. This provides a reference point, allowing for the calculation of absolute entropy by measuring entropy changes relative to this zero point using thermodynamical data.</p> Signup and view all the answers

Suppose the standard enthalpy of formation ($\Delta_fH^0$) for a particular element in a non-standard state is non-zero. Explain what this implies about the stability of the element in that non-standard state compared to its reference state.

<p>If the standard enthalpy of formation ($\Delta_fH^0$) of an element in a non-standard state is non-zero, it implies that the element in its reference state is more stable than in the non-standard state. A non-zero value suggests that energy is either required (positive) or released (negative) when converting from the reference state to the non-standard state.</p> Signup and view all the answers

Define Gibbs energy (G) and explain its significance in determining the spontaneity of a reaction.

<p>Gibbs energy (G) represents the maximum amount of energy available from a system to do useful work at constant temperature and pressure. It is defined as G = H - TS. A negative change in Gibbs energy (∆G &lt; 0) indicates a spontaneous process, while a positive change (∆G &gt; 0) indicates a non-spontaneous process.</p> Signup and view all the answers

Derive the relationship between the change in Gibbs energy (∆G), change in enthalpy (∆H), and change in entropy (∆S) at constant temperature.

<p>Starting with G = H - TS, at constant temperature, the change in Gibbs energy is derived as ∆G = ∆H - T∆S, where ∆H is the change in enthalpy, T is the temperature, and ∆S is the change in entropy.</p> Signup and view all the answers

For the reaction: $N_2(g) + 3H_2(g) \rightarrow 2NH_3(g)$, what information is needed to calculate the standard reaction enthalpy using standard enthalpies of formation?

<p>To calculate the standard reaction enthalpy, we need the standard enthalpies of formation ($\Delta_fH^0$) of all reactants and products. Specifically, we need the $\Delta_fH^0$ for $N_2(g)$, $H_2(g)$, and $NH_3(g)$.</p> Signup and view all the answers

A bomb calorimeter measures heat at constant volume. How is the heat measured in a bomb calorimeter related to the change in internal energy ($\Delta U$) of the system?

<p>In a bomb calorimeter, the heat measured at constant volume ($q_v$) is equal to the change in internal energy ($\Delta U$) of the system. This is because, at constant volume, no work is done ($w = 0$), so all the heat goes into changing the internal energy.</p> Signup and view all the answers

Describe the conditions under which a reaction is always spontaneous in terms of ∆H and ∆S.

<p>A reaction is always spontaneous when the change in enthalpy (∆H) is negative and the change in entropy (∆S) is positive. This ensures that ∆G is always negative, regardless of temperature.</p> Signup and view all the answers

Explain how temperature influences the spontaneity of a reaction when both ∆H and ∆S are positive.

<p>When both ∆H and ∆S are positive, the spontaneity of a reaction depends on temperature. The reaction will be spontaneous at high temperatures, where the T∆S term is greater than ∆H, resulting in a negative ∆G.</p> Signup and view all the answers

Consider two reactions: (1) $A \rightarrow B$ with $\Delta rH = -50 kJ/mol$ and (2) $X \rightarrow Y$ with $\Delta rH = +25 kJ/mol$. Which reaction is more favorable thermodynamically at standard conditions, and why?

<p>Reaction (1) $A \rightarrow B$ is more favorable thermodynamically. A negative $\Delta rH$ indicates that the reaction is exothermic, meaning it releases heat and leads to a lower energy state for the products compared to the reactants, making it more spontaneous than the endothermic Reaction (2).</p> Signup and view all the answers

Explain the significance of the reference state in the context of standard enthalpy of formation. Why is it important to define a reference state.

<p>The reference state provides a common baseline for comparing the relative stability of different compounds. Defining a reference state (the most stable form of an element at standard conditions) allows for a consistent assignment of zero enthalpy to elements in their standard states. This makes it possible to calculate and compare the enthalpy changes of various reactions.</p> Signup and view all the answers

For a reaction at equilibrium, what is the value of ∆G and how does it relate to the total entropy change of the system and surroundings?

<p>At equilibrium, the change in Gibbs energy (∆G) is zero. This corresponds to a state where the total entropy change (∆S_total) of the system and surroundings is also zero, indicating no net tendency for the reaction to proceed in either direction.</p> Signup and view all the answers

Contrast the behavior of spontaneous vs. non-spontaneous processes in terms of both $\Delta G_{syst}$ and $\Delta S_{total}$.

<p>For a spontaneous process, $\Delta G_{syst}$ is negative and $\Delta S_{total}$ is positive. Conversely, for a non-spontaneous process, $\Delta G_{syst}$ is positve and $\Delta S_{total}$ is negative.</p> Signup and view all the answers

Flashcards

Thermodynamics

Deals with the relationship between heat and work.

System (Thermodynamics)

The part of the universe under observation.

Surroundings

The part of the universe outside the system.

Open System

System that exchanges both energy and matter with surroundings.

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Closed System

System that exchanges energy but not matter.

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Isolated System

System that exchanges neither energy nor matter.

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Extensive Properties

Properties that depend on the amount of matter.

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Intensive Properties

Properties independent of the amount of matter.

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Cv

Heat capacity at constant volume.

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Cp

Heat capacity at constant pressure.

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Relationship between Cp and Cv

Cp - Cv = R, where R is the ideal gas constant.

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Reaction Enthalpy (ΔrH)

The enthalpy change during a chemical reaction.

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Calculating ΔrH

ΔrH = (sum of product enthalpies) – (sum of reactant enthalpies)

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Standard Enthalpy of Reaction (ΔrH0)

Enthalpy change when all substances are in their standard states (1 bar pressure and 298 K).

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Standard Enthalpy of Formation (ΔfH0)

Enthalpy change for forming one mole of a compound from its elements in their most stable state.

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Calculating ΔrH0

ΔrH0 = ∑ ΔfH0(products) - ∑ ΔfH0(reactants)

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Work (non-expansion)

Wnon-exp = E x Q

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Sign Convention for Work

Work done on the system is positive, work done by the system is negative.

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Free Expansion

Expansion of a gas into a vacuum where external pressure is zero.

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Internal Energy (U)

The total energy possessed by a body due to molecular motion and interactions.

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First Law of Thermodynamics

Energy cannot be created or destroyed, only converted from one form to another. ΔU = q + w

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ΔU at Constant Volume

At constant volume, the change in internal energy equals the heat transfer: ΔU = qv.

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Enthalpy (H)

The total heat content of a system. H = U + PV

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Enthalpy Change (ΔH)

ΔH = ΔU + PΔV. Enthalpy change equals the change in internal energy plus the product of pressure and volume change.

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Enthalpy of Phase Transition

The enthalpy change when one mole of a substance transitions from one phase to another at a specific temperature.

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Enthalpy of Fusion (ΔfusH0)

The enthalpy change when one mole of a solid becomes a liquid at its melting point. Always positive (endothermic).

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Enthalpy of Vaporization (ΔvapH0)

The enthalpy change when one mole of a liquid becomes a gas at its boiling point.

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Enthalpy of Sublimation (ΔsubH0)

The enthalpy change when one mole of a solid directly becomes a gas below its melting point.

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Hess’s Law

The total enthalpy change for a process is the same, whether it occurs in one step or multiple steps.

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Thermochemical Equation

A balanced chemical equation that includes the enthalpy change of the reaction. Physical states are specified.

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Standard Enthalpy of Combustion (ΔcH0)

The enthalpy change when one mole of a substance is completely burned in excess oxygen under standard conditions. Always negative (exothermic).

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Spontaneous Process

A process that occurs on its own without external input.

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Non-spontaneous Process

A process needing continuous external influence to occur.

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Spontaneous Chemical Reactions

Reactions that occur without continuous external energy input.

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Entropy (S)

A measure of the disorder or randomness within a system.

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Change in Entropy (∆S)

The change in entropy is the difference between final and initial entropy values: ∆S = S2 – S1

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Entropy Change Equation

∆S = qrev/T, where qrev is heat absorbed reversibly and T is temperature.

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Spontaneity and Entropy

For a spontaneous process, the total entropy change of the system and surroundings is positive: ∆STotal > 0.

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Second Law of Thermodynamics

The entropy of the universe always increases during every spontaneous process.

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Third Law of Thermodynamics

Entropy of a perfectly crystalline substance is zero at absolute zero.

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Gibb's Energy (G)

Maximum energy available from a system to do useful work.

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Gibb's Equation

∆G = ∆H - T∆S; relates Gibb's energy change to enthalpy, temperature, and entropy changes.

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Spontaneous Process (∆G)

∆Gsyst < 0

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Non-Spontaneous Process (∆G)

∆Gsyst > 0

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Equilibrium (∆G)

∆Gsyst = 0

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Always Spontaneous

∆H < 0 and ∆S > 0

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Always Non-Spontaneous

∆H > 0 and ∆S < 0

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Study Notes

  • Thermodynamics is the study of the relationship between heat and work, particularly heat changes in chemical reactions

Systems and Surroundings

  • The system is the part of the universe under observation, while the surroundings are everything else
  • A boundary, real or imaginary, separates the system from its surroundings
  • The universe is the sum of the system and its surroundings
  • Systems are classified based on their ability to exchange energy and matter
  • An open system exchanges both energy and matter with the surroundings like hot water in an open vessel
  • A closed system exchanges only energy, not matter with the surroundings, like hot water in a closed vessel
  • An isolated system exchanges neither energy nor matter with the surroundings, like hot water in a thermos flask
  • Microscopic systems contain few particles, while macroscopic systems contain many
  • Macroscopic properties include temperature (T), pressure (P), volume (V), length (l), breadth (b), height (h), internal energy (U), enthalpy (H), entropy (S), and Gibb's energy (G)

Extensive vs. Intensive Properties

  • Extensive properties depend on the amount of matter, such as volume (V), length (l), breadth (b), height (h), internal energy (U), enthalpy (H), entropy (S), Gibb's energy (G), and heat capacity
  • Intensive properties are independent of the amount of matter, such as temperature (T), pressure (P), volume (V), density, refractive index, molar heat capacity, viscosity, and surface tension

State and Path Functions

  • State functions depend only on the initial and final states (e.g., T, P, V, U, H, S, G)
  • Path functions depend on the path taken (e.g., heat (q) and work (w))

Thermodynamic Processes

  • A process occurs when a state changes in a system
  • Isothermal: constant temperature (∆T = 0, ∆q ≠ 0)
  • Isobaric: constant pressure (∆P = 0)
  • Isochoric: constant volume (∆V = 0)
  • Adiabatic: no heat exchange (∆q = 0, ∆T ≠ 0)
  • Cyclic: system returns to its initial state (∆U = 0, ∆H = 0)
  • Reversible processes involve infinitesimally small differences between driving and opposing forces
  • Irreversible processes occur with large differences in forces and proceed in one direction

Heat and Work

  • Heat is energy that flows from a hot body to a cold body
  • Heat absorbed by a system is positive (+ve), heat evolved is negative (-ve)
  • Work includes expansion work and non-expansion work
  • Expansion work (Wexp) relates to gaseous systems
  • Wexp = -P∆V for irreversible processes
  • = -2.303nRT log(V2/V1) for reversible processes
  • Non-expansion work (Wnon-exp) relates to electrochemical cells, Wnon-exp = E x Q
  • Work done on the system is positive (+ve), work done by the system is negative (-ve)
  • Free expansion into a vacuum involves no work (external pressure = 0)

Internal Energy

  • A body's internal energy (U) is the sum of its molecular energies
  • Internal energy is an extensive property and a state function
  • The change in internal energy (∆U) can be calculated using a Bomb Calorimeter: ∆U = U2 - U1
  • Internal energy changes by heat transfer or work
  • First law of thermodynamics: energy is conserved (∆U = q + w)
  • For solids/liquids, ∆V = 0, so ∆U = q
  • For isothermal reversible processes, ∆U = 0, thus q = -w = 2.303nRT log V2/V1
  • For adiabatic processes, q = 0, thus ∆U = w
  • At constant volume, ∆V = 0, so ∆U = qv, it represents heat absorbed/evolved

Enthalpy

  • Enthalpy (H) is the total heat content, the sum of internal energy and pressure-volume energy: H = U + PV
  • It's a state function and extensive property; change in enthalpy depends only on initial and final states (∆H = H2 - H1)
  • Enthalpy is measured in kJ/mol using a calorimeter
  • For a reaction, ∆H = Hp - HR, where Hp is the enthalpy of products and HR is that of reactants
  • Positive ∆H indicates an endothermic process (heat absorbed)
  • Negative ∆H indicates an exothermic process (heat evolved)

Relation between ΔH and ΔU

  • For a gaseous reaction at constant P & T: ∆H = ∆U + P∆V
  • Using the ideal gas equation, PV = nRT, ∆H = ∆U + ∆nRT, where ∆n = n(products) - n(reactants)
  • If ∆n = 0, then ∆H = ∆U
  • If ∆n > 0, then ∆H > ∆U
  • If ∆n < 0, then ∆H < ∆U
  • At constant pressure ∆H = qp, where qp is the heat evolved or absorbed

Heat Capacity

  • Heat capacity (C) is the heat needed to raise the temperature of a body by 1°C or 1K
  • C = q/∆T
  • Specific heat capacity is the amount of heat to raise the temperature of a unit mass of a body through 1°C or 1K
  • Molar heat capacity is the amount of heat to raise the temperature of 1 mole of a substance through 1°C or 1K
  • At constant volume, qv = ∆U = Cv∆T
  • At constant pressure, qp = ∆H = Cp∆T
  • For 1 mole of an ideal gas, ∆H = ∆U + R∆T
  • Thus, Cp = Cv + R, or Cp - Cv = R

Enthalpy Change of a Reaction

  • Reaction enthalpy (∆H) is the enthalpy change during a chemical reaction
  • ∆H = (sum of enthalpies of products) – (sum of enthalpies of reactants), or ∆H = ΣHp - ΣHR

Standard Enthalpy

  • Standard enthalpy of reaction (∆H°) is the enthalpy change when all substances are in their standard states (1 bar, 298 K)
  • Standard enthalpy of formation (∆fH°) is the enthalpy change for forming 1 mole of a compound from its elements in their most stable state (reference state)
  • The reference state of an element is its most stable state at 25°C and 1 bar pressure; its ∆fH° is zero by convention
  • Std. enthalpy of reaction = Sum of the standard enthalpies of formation of products – Sum of the std. enthalpies of formation of reactants

Enthalpies of Phase Transition

  • Enthalpy of fusion (∆fusHº) is the enthalpy change for a solid to liquid at its melting point
  • Enthalpy of vaporization (∆vapHº) is the enthalpy change for a liquid to vapor at its boiling point
  • Enthalpy of sublimation (∆subHº) is the enthalpy change for a solid directly to gas below its melting point

Hess's Law

Hesses's Law of Constant Heat Summation states that the total enthalpy change is the same whether the reaction occurs in one or several steps.

  • Standard reaction enthalpy is the sum of the standard enthalpies of the intermediate reactions

Thermochemical Equations

Thermochemical Equations are balanced chemical equations include the enthalpy of reaction with the physical states of reactants and products

Standard Enthalpy of Combustion

  • Standard enthalpy of combustion (∆cH°) the enthalpy change when 1 mole of a substance is completely burnt in excess of air or oxygen in their standard states; it is always negative (exothermic)

Enthalpy of Atomization

  • Enthalpy of atomization (∆aH°) is the enthalpy change when breaking one mole of bonds completely to obtain atoms in the gas phase
  • Bond Enthalpy is the same as the enthalpy of atomization (∆bondH°) for a diatomic molecules
  • Chemical reactions involve bond breaking (endothermic) and bond making (exothermic)
  • The bond dissociation enthalpy average for polyatomic molecules since bonds differ
  • The standard enthalpy of reaction, ΔH^0, relates to reactant and product bond enthalpies in gas phase reactions

Enthalpy of Solution

  • Enthalpy of solution (∆solH°) is the enthalpy change when one mole of a substance is dissolved in a specified amount of solvent. and determined by the lattice enthalpy (∆latticeHº)and enthalpy of hydration of ions (∆hydHº)

Lattice Enthalpy

  • Lattice enthalpy (∆latticeH°) of an ionic compound is the enthalpy change when one mole an ionic compound dissociates into gaseous ions.
  • Borne-Haber Cycle used as an indirect method to calculate lattice enthalpies since we cannot determine lattice enthalpies directly by experiment.

Enthalpy of Dilution

  • Enthalpy of dilution (∆dilHº): depends on the volume and concentration added when a solution is diluted with solvent

Spontaneous Process

  • A spontaneous process occurs without external help; a non-spontaneous process requires external help
  • Spontaneity is favored by decreasing energy and increasing disorder (entropy)

Entropy

  • Entropy (S) measures the degree of disorder or randomness, being an extensive property and a state function
  • For amount ‘q’ heat absorbed reversibly at temp T, then the change in entropy, ∆S=fraction quantity rev/Temperature
  • During a spontaneous process, disorder and entropy increase becoming positive thus we know that the total entropy for system and surroundings, ASTotal = ∆S sys+ ∆S surr

Laws of Thermodynamics

  • Second Law: The entropy of the universe increases in every spontaneous process
  • Third Law: The entropy of perfectly crystalline substances is zero at absolute zero

Gibb's Energy

  • Gibbs' can be defined as the maximum amount of available energy that can be converted to useful work; given by the equations, G= H - TS
  • Gibbs' Energy is extensive property, is given by the Gibb's Equation
  • We can use the Gibbs Equation to know that the Conditions for ∆G to be negative are if ∆H is -ve and ∆S +ve, then vice versa.
  • In Gibb's energy changes (∆G) and Equilibrium constant (K) are related, the (A, Go) is related to equilibrium constant with the given equation A, G° = -RT InK

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Discussions on system types (isolated, closed, open), properties (extensive, intensive), state vs path functions, and macroscopic changes due to energy transfer.

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