AP®︎ Chemistry: Unit 6 Flashcards

Master key terms and definitions for Unit 6 of AP Chemistry – Thermochemistry to help you prep for quizzes and the AP exam.


0%
70 cards total
70 not started
0 learning
0 almost done
0 mastered
Term

Energy

Definition

The capacity to do work or transfer heat.

1 / 70
Energy
Not Started

The capacity to do work or transfer heat.

6.1.A
Kinetic Energy
Not Started

Energy due to motion; in particles, it increases as temperature increases.

6.1.A6.1.A.1
Potential Energy
Not Started

Stored energy due to position or interactions, especially in chemical bonds and attractions.

6.1.A6.1.A.3
Physical and Chemical Transformations as Endothermic or Exothermic
Not Started

Heating, cooling, phase changes, and reactions can absorb or release energy.

6.1.A6.1.A.2
Dissolution as Endothermic or Exothermic
Not Started

Solution formation absorbs or releases energy depending on relative interaction strengths before and after dissolving.

6.1.A6.1.A.4
Temperature Change and Energy Transfer
Not Started

Temperature changes show energy transfer between system and surroundings during physical or chemical changes.

6.1.A6.1.A.1
First Law Of Thermodynamics
Not Started

Energy is conserved: it cannot be created or destroyed, only transferred or converted between forms.

6.1.A6.1.A.3
System And Surroundings
Not Started

The system is the part being studied, such as the reacting chemicals; the surroundings are everything else that can exchange energy with it.

6.1.A6.1.A.3
Energy Diagram / Potential Energy Diagram
Not Started

A graph of energy versus reaction progress showing reactants, products, and any energy barrier.

6.2.A6.2.A.1
Axes of an Energy Diagram
Not Started

Vertical axis is potential energy; horizontal axis is reaction or process progress.

6.2.A6.2.A.1
Potential Energy of Reactants and Products
Not Started

The starting and ending energy levels shown for substances before and after a process.

6.2.A6.2.A.1
Activated Complex / Transition State
Not Started

The highest-energy, least stable arrangement of atoms at the top of the energy barrier.

6.2.A
Representing Phase Changes with Energy Diagrams
Not Started

Physical changes can be graphed like reactions, showing energy absorbed or released during phase change.

6.2.A6.2.A.1
Latent Heat
Not Started

Energy absorbed or released during a phase change without a temperature change.

6.2.A
Activation Energy
Not Started

The energy difference between the reactants and the peak, equal to the minimum energy needed to react.

6.2.A
Endothermic Vs. Exothermic On An Energy Diagram
Not Started

On an energy diagram, exothermic processes have products lower in enthalpy than reactants and a negative ΔH, while endothermic processes have products higher than reactants and a positive ΔH.

6.2.A6.2.A.1
Phase Changes: Endothermic Vs. Exothermic
Not Started

Melting, vaporization, and sublimation are endothermic and absorb energy; freezing, condensation, and deposition are exothermic and release energy.

6.2.A6.2.A.1
Thermal Contact
Not Started

A condition where two bodies can exchange energy through collisions between their particles.

6.3.A6.3.A.2
Direction Of Heat Flow
Not Started

Energy as heat flows from the warmer body to the cooler body.

6.3.A
No Net Energy Transfer At Thermal Equilibrium
Not Started

Energy still moves both ways, but equal transfers cause no overall change.

6.3.A6.3.A.3
Zeroth Law Of Thermodynamics
Not Started

If A is in thermal equilibrium with B, and B with C, then A with C.

6.3.A
Heat Transfer Through Molecular Collisions
Not Started

Collisions transfer kinetic energy from faster particles to slower particles in thermal contact.

6.3.A6.3.A.2
Thermal Equilibrium
Not Started

Thermal equilibrium is the state in which objects in thermal contact have the same temperature and average kinetic energy, so no net heat is transferred between them.

6.3.A6.3.A.3
Calorimetry
Not Started

The measurement of heat transfer by tracking temperature changes in an insulated system.

6.4.A6.4.A.1
Heat Transfer Equation
Not Started

q = mcΔT, where heat equals mass times specific heat times temperature change.

6.4.A6.4.A.1
Specific Heat Capacity
Not Started

The heat required to raise 1 gram of a substance by 1 degree Celsius.

6.4.A6.4.A.5
Heat Capacity and Molar Heat Capacity
Not Started

Heat capacity is heat per degree for an object; molar heat capacity is heat per degree per mole.

6.4.A6.4.A.5
Temperature Change
Not Started

The difference between final and initial temperature, calculated as Tfinal minus Tinitial.

6.4.A
Heat Lost Equals Heat Gained
Not Started

In an isolated calorimeter, energy released by one part equals energy absorbed by another.

6.4.A6.4.A.2
Sign of q in Heating and Cooling
Not Started

Positive q means heat is absorbed; negative q means heat is released.

6.4.A6.4.A.4
Specific Heat and Temperature Change Relationship
Not Started

For equal heat and mass, a larger specific heat gives a smaller temperature change.

6.4.A6.4.A.3
Solving for Unknown Specific Heat
Not Started

Set heat lost equal to heat gained, then solve q = mcΔT for c.

6.4.A6.4.A.1
Energy Changes in Chemical Systems
Not Started

Systems change energy through heating or cooling, phase changes, and chemical reactions.

6.4.A6.4.A.6
Coffee-Cup Calorimetry
Not Started

An insulated constant-pressure setup where measured heat equals the reaction’s enthalpy change.

6.4.A6.4.A.1
Dissolution Calorimetry
Not Started

A calorimetry method using solution temperature changes to identify heat flow during dissolving.

6.4.A6.4.A.7
Heating Curve
Not Started

A graph of temperature versus heat added showing warming slopes and flat phase-change plateaus.

6.5.A6.5.A.1
Cooling Curve
Not Started

A graph of temperature versus heat removed showing cooling slopes and flat phase-change plateaus.

6.5.A6.5.A.1
Constant Temperature During a Phase Change
Not Started

A pure substance’s temperature stays unchanged while added or removed energy changes its phase.

6.5.A6.5.A.1
Molar Enthalpy of Fusion and Vaporization
Not Started

The energy per mole required to melt or vaporize a substance at constant temperature.

6.5.A
Complementary Phase-Change Enthalpies
Not Started

Opposite phase changes have equal magnitudes and opposite signs, such as vaporization and condensation.

6.5.A6.5.A.2
Phase-Change Heat Calculation
Not Started

Use q = nΔH for phase changes, with moles times the molar enthalpy.

6.5.A
Heating and Cooling Curve Calculations
Not Started

Use q = mcΔT on slopes and q = nΔH or mH on plateaus, then sum steps.

6.5.A
Heat of Vaporization vs Heat of Fusion
Not Started

Vaporization usually requires more energy than melting because more intermolecular attractions must be overcome.

6.5.A
Molar Enthalpy of Condensation and Freezing
Not Started

The energy released per mole when a gas condenses or a liquid freezes.

6.5.A6.5.A.2
Molar Enthalpy of Reaction
Not Started

Enthalpy change per mole of reaction as written in the balanced equation, usually in kJ/mol.

6.6.A
Heat / q
Not Started

Thermal energy transferred between a system and surroundings, measured in joules or kilojoules.

6.6.A
q = nΔH
Not Started

Calculate reaction heat by multiplying moles of reacting substance by molar enthalpy change.

6.6.A
Calculating Moles from Heat and ΔH
Not Started

Rearrange q = nΔH to n = q/ΔH, keeping units and signs consistent.

6.6.A
Limiting Reactant in Enthalpy Calculations
Not Started

Use the moles of the limiting reactant to determine the total heat of reaction.

6.6.A
Thermal Equilibrium After a Reaction
Not Started

Energy is exchanged until products and surroundings reach the same final temperature.

6.6.A6.6.A.2
Potential Energy to Kinetic Energy in Reactions
Not Started

Differences in chemical potential energy appear as particle kinetic energy changes and temperature changes.

6.6.A6.6.A.3
Constant Pressure and Enthalpy
Not Started

At constant pressure, the reaction enthalpy change equals the heat transferred, q.

6.6.A6.6.A.3
Enthalpy
Not Started

A thermodynamic quantity representing a system’s heat content at constant pressure; enthalpy change, ΔH, is the difference between final and initial enthalpy values.

6.6.A6.6.A.3
Endothermic And Exothermic Processes
Not Started

Endothermic processes absorb heat from the surroundings and have positive ΔH; exothermic processes release heat to the surroundings and have negative ΔH.

6.6.A6.6.A.1
Enthalpy Change Of Reaction
Not Started

The overall enthalpy change, ΔH, is the difference between products and reactants; for a reaction at constant pressure, it is the heat absorbed or released.

6.6.A6.6.A.1
Bond Order and Bond Strength
Not Started

Triple bonds are strongest, double bonds intermediate, and single bonds weakest, with increasing bond enthalpy.

6.7.A
Bond Length and Bond Strength
Not Started

Shorter bonds are generally stronger and have higher bond enthalpies than longer, weaker bonds.

6.7.A
Counting Bonds in a Reaction
Not Started

Draw reactant and product structures, count each bond type, then apply the bond enthalpy equation.

6.7.A6.7.A.2
Average Bond Enthalpy
Not Started

The average energy needed to break one mole of a specific gas-phase bond.

6.7.A6.7.A.2
Reaction Enthalpy from Bond Energies
Not Started

Subtract bond energies of bonds formed from bonds broken to estimate reaction enthalpy.

6.7.A6.7.A.2
Bond Energy Changes In Reactions
Not Started

Breaking bonds absorbs energy, while forming bonds releases energy; these changes alter chemical potential energy and contribute to the reaction enthalpy.

6.7.A6.7.A.1
Enthalpy of Reaction from Enthalpies of Formation
Not Started

Calculate using ΣnΔHf°(products) minus ΣmΔHf°(reactants), including stoichiometric coefficients.

6.8.A6.8.A.1
Stoichiometric Coefficients in ΔH°rxn Calculations
Not Started

Multiply each substance’s formation enthalpy by its balanced-equation coefficient before summing.

6.8.A6.8.A.1
Physical State in ΔHf° Tables
Not Started

Use the value matching the substance’s phase, since liquids, gases, and solids have different values.

6.8.A6.8.A.1
Standard Enthalpy of Formation
Not Started

Enthalpy change when one mole of a compound forms from elements in standard states.

6.8.A
Standard States and Elemental ΔHf°
Not Started

Elements in their most stable standard states have standard enthalpies of formation equal to zero.

6.8.A
Representing a Process as a Sequence of Steps
Not Started

Break an overall reaction into known reactions, then manipulate and add them to match the target.

6.9.A6.9.A.1
Rules of Hess's Law
Not Started

Reverse reaction: change ΔH sign; multiply coefficients: scale ΔH; add reactions: add ΔH values.

6.9.B6.9.B.2
Canceling Intermediate Species
Not Started

Species appearing on both sides of added steps cancel, leaving only the overall reaction.

6.9.A6.9.A.1
Hess's Law
Not Started

The overall enthalpy change equals the sum of step enthalpies because energy is conserved.

6.9.B6.9.B.1