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Chapter 7: Thermochemistry and Thermodynamics – Study Notes

Study Guide - Smart Notes

Tailored notes based on your materials, expanded with key definitions, examples, and context.

Thermodynamics: Key Concepts

Introduction to Thermodynamics

Thermodynamics is the study of energy changes, particularly heat and work, that accompany chemical and physical processes. It provides a framework for understanding how energy is transferred within a system and between a system and its surroundings.

  • System: The part of the universe under study (e.g., a chemical reaction in a beaker).

  • Surroundings: Everything outside the system that can exchange energy with it.

  • Universe: The sum of the system and its surroundings.

Key Principle: The total energy of the universe is constant. Energy lost by the system is gained by the surroundings and vice versa.

  • Energy Conservation: $\Delta E_{sys} = -\Delta E_{surr}$

Energy changes are tracked using sign conventions:

Energy

System (Sign)

Change for System

Surroundings (Sign)

Change for Surroundings

q (heat)

+

Absorbing heat (Endothermic)

-

Losing heat

q (heat)

-

Losing heat (Exothermic)

+

Absorbing heat

w (work)

+

Work done on system (decreasing volume)

-

Doing work (increasing volume)

w (work)

-

Work done by system (increasing volume)

+

Work done on surroundings (decreasing volume)

ΔE (internal energy)

+

Gaining energy

-

Losing energy

ΔE (internal energy)

-

Losing energy

+

Gaining energy

Internal Energy and Calculations

Internal Energy (ΔE)

Internal energy is the total energy contained within a system. It can be changed by heat (q) and work (w):

  • Formula: $\Delta E = q + w$

Example Problems:

  • Calculate the change in internal energy for a gas in a piston if the gas absorbs 5.973 kJ of heat and does 0.589 kJ of work by pushing the piston.

  • Determine the work done by a system if a balloon loses 206 J of heat and the overall change in internal energy is +458 J. Did the balloon expand or contract?

Heat Capacity and Calorimetry

Heat Capacity

Heat capacity is a measure of the amount of heat required to change a system's temperature by a given amount.

  • Specific Heat (c): The amount of heat required to raise the temperature of 1 gram of a substance by 1°C.

  • Formula: $q = m \times C_s \times \Delta T$

Example Calculations:

  • How much heat is required to warm 420.0 grams of ethylene glycol from 22.2°C to 100.0°C? ($C_{s, ethylene\ glycol} = 2.78 \ J/g^\circ C$)

  • What is the final temperature of a lump of gold (5.009 g, $C_{s, Au} = 0.129 \ J/g^\circ C$) after absorbing 11.04 J of heat energy?

  • Calculate the heat absorbed by 1.0 tablespoon of chicken broth (assume $C_{s, broth} = 4.184 \ J/g^\circ C$) when heated from 22.2°C to 100.0°C.

  • Determine the change in temperature for a 63.1 g silver spoon ($C_{s, Ag} = 0.240 \ J/g^\circ C$) if it absorbs the same heat as the broth above.

  • Find the mass of a hot piece of iron ($C_{s, Fe} = 0.449 \ J/g^\circ C$) placed in 200 g of water ($C_{s, H_2O} = 4.184 \ J/g^\circ C$) when equilibrium is reached at 28.1°C (initially 275.8°C for iron, 22.2°C for water).

Pressure-Volume Work

Work Done by Expanding Gases

Pressure-volume (PV) work occurs when a system changes volume against an external pressure.

  • Formula: $w = -P_{ext} \Delta V$

  • Conversion: $1.00 \ atm \cdot L = 101.31 \ J$

Example: Calculate the work done (in Joules) by inflating a balloon from 2.0 L to 3.8 L on the moon where the atmospheric pressure is 0.00500 atm.

Calorimetry: Measuring Energy Changes

Constant Volume Calorimetry (Bomb Calorimeter)

Bomb calorimetry measures the change in internal energy (ΔE) at constant volume. All energy from the reaction is converted to heat because $\Delta V = 0$.

  • Calorimeter is isolated: matter cannot leave, and no heat is exchanged with the outside.

  • Relationship: $q_{rxn} = -q_{calorimeter}$ (no heat is lost to the surroundings).

Bomb calorimeter diagram

Example Calculations:

  • Determine $\Delta E_{rxn}$ for the combustion of ethanol if a 1.015 g sample causes the calorimeter temperature to rise from 22.8°C to 35.2°C. The calorimeter has a heat capacity of 5.936 kJ/°C.

  • Find $\Delta E_{rxn}$ for the combustion of methanol (1.015 g, temperature change 21.4°C to 34.0°C, calorimeter heat capacity 4.90 kJ/°C).

  • Calculate the calorimeter constant ($C_{cal}$) if 1.009 g of butane causes a 10.6°C temperature change. ($\Delta E_{rxn}$ for butane combustion = -2878 kJ/mol).

Constant Pressure Calorimetry (Coffee Cup Calorimeter)

Used for reactions open to the atmosphere (constant pressure). Measures enthalpy change ($\Delta H$) rather than internal energy ($\Delta E$).

  • Cannot assume all work is zero; $\Delta E$ is related to $q_p$ (heat at constant pressure).

Enthalpy (H) and Enthalpy Change (ΔH)

Definition and Equations

Enthalpy is a thermodynamic property that represents the heat absorbed or released at constant pressure.

  • Formula: $H = E + PV$

  • Enthalpy Change: $\Delta H = \Delta E + P \Delta V$

  • If $\Delta V$ is negligible, $\Delta H \approx \Delta E$

Example: The reaction of sodium and water produces 367.5 kJ of heat and does 2.5 kJ of work. Calculate $\Delta H$ and $\Delta E$ for the reaction.

Coffee Cup Calorimetry and Enthalpy

For aqueous reactions, $\Delta H_{rxn}$ can be determined using constant pressure calorimetry. The sign conventions for system and surroundings are important for interpreting results.

System

Surroundings

q = -

q = +

q = +

q = -

Summary Table: Exothermic vs. Endothermic Processes

Process

System (q)

System (T)

Calorimeter (q)

Calorimeter (T)

Exothermic

-

Decreases

+

Increases

Endothermic

+

Increases

-

Decreases

Key Equations

  • $\Delta E = q + w$

  • $q = m \times C_s \times \Delta T$

  • $w = -P_{ext} \Delta V$

  • $H = E + PV$

  • $\Delta H = \Delta E + P \Delta V$

Additional info:

  • Thermochemistry is a branch of thermodynamics that specifically studies the heat involved in chemical and physical changes.

  • Calorimetry is a practical technique for measuring heat changes in the laboratory.

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