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define internal energy
sum of the randomly distributed kinetic energies and potential energies of the particles in a body
internal energy of a system is increased when
energy is transferred to it
by heating or when work is done on it
during a state change
potential energies of particles changing
kinetic energies do not change
specific heat capacity
Q = mc delta theta
the energy required to raise the temperature 1kg of a substance by 1K
specific latent heat
Q = ml
when temperatures is changing
kinetic energy is changing
potential energy is constant
how atoms change their arrangement during melting or boiling
energy transferred into system reduces the number of nearest atomic partners / atoms move their centre of vibration
how motion of the atoms changes during temperature rise
mean kinetic energy of the atoms increases so their mean speed increases
specific latent heat of fusion
energy required to change a unit mass of a substance from the solid state to the liquid state or vice versa
without temperature change
temperature increase of air when speed of pump is higher
greater work done on air molecules
increases mean speed of articles and mean square speed
therefore increases kinetic energy and temperature by 1st law of thermodynamics
pressure
force per unit area that it exerts normally to the surfaces of a container
ideal gases
potential energies between particles assumed to be 0
boyle’s law
pressure is inversely proportional to the volume at a constant temperature for a fixed mass of gas
P1V1=P2V2
isothermal - any change at a constant temperature
charles’s law
volume is proportional to its temperature at a constant pressure for a fixed mass of gas
T1V1=T2V2
isobaric - any change at a constant pressure
pressure law
the pressure is directly proportional to its temperature at a constant volume for a fixed mass of gas
T1P1=T2P2
isochoric - any change at a constant volume
absolute 0
temperature at which kinetic energy of the particles is 0
0k which is -273.15 celsius
a state of minimum internal energy
degrees to kelvin
+273
thermal equilibrium
no overall heat transfer occurs between two objects at the same temperature
work done on a gas at a constant pressure
W=PΔV
number of moles, n in a mass
n = mass / molar mass
(molar mass is the mass of. mole)
number of molecules N
N = n x avogadro constant
ideal gas equation for number of moles
PV = nRT
R is gas constant 8.31 Jmol^-1K^-1
T is temperature in kelvin
n is number of moles
ideal gas equation of number of molecules
PV = NkT
k is boltzmann constant
T is temperature in kelvin
N is number of molecules
brownian motion
smoke particles moving in random motion
movement of smoke particles caused by collisions with randomly moving air molecules
smoke particles are visible but air particles are not hence air molecules must be very small
smoke particles are continuously moving because the air molecules are continuously moving