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1st law of thermodynamics
the overall change in the energy of a system during a process is due to an exchange of heat and/or work with the surrounding
delta U= q+w
Law of conservation of energy
energy cannot be created or destroyed
The energy of a system can only be changed by the
transfer of heat or work between system and surroundings
At constant volume
work is equal to zero
change in energy (delta U) = heat exchange in the surroundings(q)
at constant pressure
delta U= q - Pdelta V
heat exhange (q) in conditions of constant pressure has a special name: enthalpy (delta H)
delta U= delta H - P(delta V)
The temperature of a gas decreases if it expands…
adiabatically
delta U and delta H are
state functions
q and w are
path functions
equation for monatomic ideal gases
(T2/T1)^(3/2) =V1/V2
The internal energy of a closed system can only be altered by
the flow of heat or work across the boundary the system and surroundings
Heat and Work are transitory, meaning that
it is not associated with initial or final states, it only appears during a change in state of the system and surroundings
q is positive(q>0)
when heat is absorbed—> energy increases. (heat is withdrawn from the surroundings and deposited into the system)
q is negative (q<0)
heat is withdrawn from the system and deposited into the surroundings
Only energy, and not work is associated with
the initial and final states of the system
Work is negative (w<0)
mass in the surroundings have been raised
Work is positive (w>0)
work done on the system —> energy increases (mass in the surroundings have been lowered)
positive q and w means
the internal energy increases
q and w are NOT
state functions (state functions are defined only by the current state of the system rather than the changes)
Energy of an isolated system
will remain constant (delta U is zero )
For any cyclical process (start and end in the same note)…
delta U is zero
for any adiabatic process
q will be 0
Two types of expansive work
reversible and irreversible
Reversible process
Infinitesimal (extremely small) change in the direction of the variable that drives the process (e.g. temperature) causes a reversal in the direction of the process
Reversible expansion
It’s slow, gradual and has internal equilibrium (Pext=P)
Irreversible process
Infinitesimal (extremely small) change of the variable that drives the process (e.g. temperature) does not change the direction of the process.
Irreversible expansion
fast and does not have internal equilibrium (Pext does not equal P)
Reversible work is always bigger than irreversible work, why?
In a reversible process entropy remains constant, and entropy is directly related to the dispersal of energy; therefore, minimizing entropy means the maximum amount of energy can be converted into work. On the other hand, in an irreversible process entropy increases.
A system that’s not in internal equilibrium
a gas that is expanding so rapidly that the exchange of energy between molecules through collisions is slow compared with the rate of expansion. (different regions of gas may have different values for density, pressure and temp)
Pext > Pgas
Volume decreases, compressed. w=-Pext(delta V)
since it’s shrinking, delta V is a negative number which is why we need the negative in front in the formula. Pressure should be in Pascals and Volume in m³
Pascals
kg/ms²
Pext< Pgas
gas expands
Pext is only infinitesimally different from P gas, a tiny change in Pext can change the direction of the volume change of the gas
reversible process
In reversible process, the volume changes infinitesimally small but it’s not zero. Which formula should we use?
wrev=- integral from v1 to v2 (PextdV)
Based on the last two questions. a small change in Pext can change the direction in volume, which implies Pext is not constant. What should we change Pext to in the previous formula?
Pgas (and if it’s behaving like an ideal gas we do nRT/V)
atm to Pa
times 101325 Pa/ 1.00 atm
recap: ice melts into water at what temperature?
0C
Lead, Silver, Copper, Iron have lower specific heat capacities than wood, water and polyethylene. What does this mean?
It doesn’t take much energy to cause the lower specific heat capacities materials to become hot than the higher values (would take a lot of energy)
this is why a copper soon get hotter way easier than a wooden spoon. This is also why water takes a long time to boil.