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Chemistry B
Thermochemistry
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Types of Energy Relevant to Chemistry
potential
chemical
nuclear
kinetic
thermal
radiant
electrical
Potential energy: energy associated with an objects
position
or
composition
Chemical
energy: energy stored in
intramolecular
and
intermolecular
bonds; released in
chemical
reactions
nuclear energy
: energy stored in the collection of
neutrons
and
protons
in the atom's
nucleus
Kinetic energy
: energy associated with the random
kinetic motion
of atom and molecules
Radiant Energy
:
energy
in the form of
radiation
Electrical Energy
: energy associated with the
flow
of
charges
System
specific part of the universe of interest in a specific
application
surroundings: things around a
system
Internal energy
the
capacity
of a system to do
work
E =
sum
of all energies
∆Esys =
Ef
-
Ei
absolute internal energy is not measurable
can measure changes in the energy of a system
system = chemical reaction
Conservation of Energy
energy of the universe is
constant
energy can't be
created
or
destroyed
Esystem
lost =
E surroundings gain
∆Esys + ∆Esurroundings = ∆Euniverse =
0
∆Esys =
-∆Esurroundings
Chemical Energy
reactants -->
products
: energy released to the surroundings (
heat
/
work
)
∆Esys =
Eproducts
-
Ereactions
<
0
∆Esurroundings =
-∆Esys
>
0
when ∆Esys is negative the system
loses
energy as
heat
/
work
to the surroundings
reactants --> products (
upwards
): energy from surroundings to system
∆Esys =
Eproducts
-
Ereactions
>
0
∆Esurroundings = -∆Esys <
0
Work and Energy
work: by or on the system is
energy transfer
that results in
macroscopic
changes in the system
w = F * D: (Joules) =
Newtons
*
meters
∆Esys = q + w:
heat transfer
+
work done
Mechanical work
w = F*∆h:
pressure
cylinder-system
w = -P∆V
1 L*atm = 101.325 J
Closed-system:
when cylinder expands ∆V is (+) (Vf - Vi)
work must be (-) because ∆Esys is (-), gas is losing energy
Heat
≠
Temperature
temperature: a
measure
of the
random
molecular
motion
in an object or substance
Ke avg = 3/2 RT
heat:
energy transfer
between
2
objects often driven by a
temperature difference
q = m*C*∆T
w =
-P∆V
Quantifying Heat
heat
(q) --> system ∆Temp
heat capacity
: (C) = amount of
heat
(q) required to raise the
temp
of entire system by
1
C
specific heat capacity
(Cs) - the amount of heat (q) needed to raise the temperature of 1 gram of the substance by 1 C
Molar heat capacity
(Cm) = same, but for 1 mol of substance
q = mC∆T = mCs∆T = nCm∆T
∆T =
Tfinal
-
Tinitial
endothermic
:
∆H
and
q
(
+
)
exothermic
:
∆H
and q (
-
)
Heat (q) +/-
positive:
gains
from surroundings
negative:
loses heat
to surrounding
work (w) +/-
positive
:
surroundings
do work on system
negative
:
system
does work on
surroundings
Change in Energy ∆E +/-
positive
: energy surroundings flow
into
system
negative
: energy flows
out
of the system into
surroundings
State functions
depends
on
the
present state
energy
is state function
heat
and
work
are not state functions
∆E =
Ef
-
Ei
pressure
,
volume
, and
temperature
are state functions
∆H = Hfinal - Hinitial
∆H = H (products) - H (reactants)
constant volume
∆E =
q
(volume)
chemical reaction at
constant volume
, ∆V =
0
Change in internal energy =
heat
exchanged when V is
constant
Constant-pressure Calorimetry
coffee cup
calorimeter
measure ∆Hrxn = q (rxn) at a
constant
pressure
heat
flows from
reactants
to
solution
or vice versa
heat of reaction has
opposite
sign from heat of solution
q (rxn) =
-q
(
solution
)
physical measurement: temperature
change
of solution ∆T
∆H = q (pressure)
Calorimetry
is the measurement of
heat
of a
reaction
(q)
physical measurement is
change
in
temperature
(∆T)
intangible quantity is
heat
(q)
Bomb Calorimeter
measures ∆Erxn = q (rxn) at a
constant
volume
heat of reaction has
opposite
sign form heat of calorimeter q (cal) =
-q
(rxn)
physical measurement: temperature change of
calorimeter
properties of enthalpies of reaction
enthalpies of reaction (∆Hrxn) are
extensive
: depends on the
amount
of reactants
∆Hxn for
backwards
reaction changes the
sign
of ∆Hrxn for
forwards
reaction (∆H2 =
- ∆H1
)
Hess's
Law
Hess's Law
∆Hrxn is the
sum
of
enthalpy change
of each step of a
stepwise reaction
(
∆Hrxn
= ∆H1 + ∆H2 + ∆H3)
state function
H is not
path-dependent
only depends on
initial
and
final states
Standard state of elements
pure
substance in its most
stable
state (Ex.
O2
,
noble gases
)
pressure of
1
atm
temperature of
25
C
Standard states of gases:
pressure
of
pure
gas at
1
atm
Standard states of liquids or solids
pure
substance in its most
stable
state
pressure of
1
atm
temperature of
25
C
standard states of solutions
concentration of exactly
1M
(moles/Liter)
Standard enthalpy
all reactants and products are at
standard
stage
pure compounds:
1
mol forms from
constituent
elements in their standard state
pure elements: the
constituent
element of an element is itself
Hf
=
0
(Ex. for O2 standard enthalpy is
0
)
Bond energy
energy associated with
breaking
a specific chemical bond
endothermic
process (
positive
∆H)
∆Hbond
>
0
Bond Enthalpy Values
in reaction, reactant bonds are
broken
and new bonds are
formed
in product
bond energy values are
averages
of bond types in all known molecules
form (
-
)
break (
+
)
bond breaking and formation
bonded
+
(break) =
+∆H
unbonded
+
bonded = -∆Hbond
Strong bond and Broken bond:
large
and
positive
∆H
Weak bond and Broken bond:
Small
and
positive
∆H
Strong and formed bond:
Large
and
negative
∆H
Weak and Formed bond:
small
and
negative
∆H