cram thermodynamics Flashcards

1
Q

isolated system

A

no exchange with environment

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

closed system

A

energy exchange with environment

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

open system

A

exchange of matter and energy with environment

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

adiabatic

A

no exchange of heat

termos, stanely cup

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

macroscopic characterization of a thermodynamic system

A

determines the state of the system by state variables

p, V and T are state variables if they describe a system in equillibrium state

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

extensive variables

A

depend on size of the system e.G energy, mass, volume, charge, entropy

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

intensive variables

A

do not depend on size e.g: pressure, temperature, concentration

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

equillibrium

A

can be reasched by spontaneous process without any outside intervention

  • properties of system do not change with time
  • intensive variables are uniformely distributed througout the system
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

non-equillibrium

A

may contain intensice variables which vary in space and time

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

internal energy

A

the energy an object or substance is due to the molecular kinetic and potential energies associated with the random motions of all the particles that make it up

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

kinetic energy

A

due to motion of the particles

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

potential energy

A

due to interactions between the atoms, ions and molecules

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

ideal gas with one atom

A

translational energy

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

ideal gas with several atomsq

A

translational and rotational and vibration energy

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

liquid and solid body

A

translational, rotational, vibration energy and attractive molecular interactions

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

elementary energy exchanges

W = y *dx

A

W = y * dx

extensive (x)
volume, matter, charge

intensive (y)

pressure
chemical potential
electric potential
temperature

product:
volumetric work
work of material transport
heat

17
Q

change of internal energy

A

sum of individual energy exchanges

18
Q

thermal interactions - > DeltaQ

A

dQ=TdS

19
Q

first law of thermodynamics

A

law of conservation of energy. energy may be converted into different forms, but the total energy of the system remains constant

20
Q

latent heat

A

Latent heat is thermal energy released or absorbed, by a body or a thermodynamic system, during a constant-temperature process. Found between change of states (from solid to liquid)

21
Q

equalization of temperature and/or pressure leads to

A

increase in entropy

22
Q

entropy in equillibrium is

A

constant

23
Q

real processes leading to equillibrium

A

1) temperature equalization
2) mixing of gases
3) conversion of macroscopic kinetic energy to thermal energy

24
Q

second law of thermodynamics

A

during spontaneous processes entropy always increases. spontaneous processes proceed towards the most pronable state

25
Q

entropy maximum

A

thermodynamic equillibrium

26
Q

statistical entropy

A

s=k*lnOmega
omega is the thermodynamic probability. thermodynamic probability is gives the number of microstates for a given macrostate

27
Q

high conformational entropy

A

random coil

28
Q

small conformational entropy

A

ordered conformations

29
Q

third law of thermodynamics

A

the entropy of one-component, crystallizing when temperature approaches zero
s=0 t=0 omega is 1

it is impossible to reach t in a finite number of steps

30
Q

usable part of internal energy at constant pressure

A

enthalpy
H=U+pV
isobaric

31
Q

usable part of internal energy at constant temperature

A

free energy

F = U-TS