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Thermodynamics
the exchange and conversion of heat energy between bodies
Kinetic energy(thermal)
K=3/2 nKbT or 3/2 nRT
n= number of particles
kb= maxwell boltzmann constant
R= universal gas constant
T = temperature
Maxwell-Bolton graph
Shows the average speed of particles throughout
Right is larger than the left, but the more scooched up it is means the more common it is
Where does thermal energy flow to
From hot to cold
How do the collisions between two gases’ molecules work
Random
Kinetic theory of gases
Gases have identical molecules unique to their certain gas
Volume is negligible
Density is constant at all point
Gas molecules exert pressure on container walls
The pressure of an ideal gas is the same everywhere
Ideal gas law
PV= NRT/Nkbt
P= Pressure
V = volume
N= number of molecules
Kb= boltzmann’s constant
T= temperature
Isochoric
Constant volume
Isothermic
Constant temperature
Isobaric
Constant pressure
Adiabatic
no heat transferred
Heating
transfer of energy into a system
Cooling
transfer of energy out of a system
Thermal equilbrium
two objects in a system/ two systems having the same temperature
Convection
heating through fluids
radioaction
heating through radioactive waves
Conduction
heating through direct contact
Internal energy(U)
Total energy of the whole system; total of each particles energy that does not have potential energy
U= Number of particles * average kinetic energy(N* Kavg)
Work on a gas
Positive during compression, negative during expansion; check same direction
W=-P(change in)V
Work by a gas
OPPOSITE DIRECTION; negative during compression, positive during expansion
Heat(Q)
thermal energy transferred from one body to another
Q = mcT
First law of thermodynamics
The change to energy is the sum of energy transferred to or from the system by heating work done of the system
U= Q + W
Insulated container
Energy does not escape
Rate of energy transfer by conduction
Q/t=kAT/L
Entropy
the amount of disorder in a system; tendency of energy to spread and the unavailability of the system to do work; highest in thermal equilibrium
Constant but can increase in a closed system
Increases when molecules/thermal energy spread out more
Isolated system
Energy stays the same