Theory that used observation about motion and energy partikel’s of substance to investigate adjective is kinetic theory of substance. Adjective that is substance adjective by all as product as flat conduct partikel’s of substance it. Kinetic theory of substance which especially used for particel’s of gas it is kinetic theory of gas.
- Definition of ideal gas
Gas which observe on this discution is ideal gas, it’s a gas have adjectives such as:
· Ideal gas to consist of particel’s (atom’s or molekul’s) wich amounth is very much and inter particel’s don’t to happen interaction.
· Each particle of gas to move with reckless aim.
· Size of gas particle can be disregard for size room.
· Each crush that to happen perfectly warped.
· Gas particle distributed to spread in all room.
· Valid
In reality no one gas to happen that egniping adjectives of ideal gas, but gas on temperature room and low press to approach adjectives of ideal gas.
- Equation state ideal gas
a. Boyle-Gay lussac law
Gas at one closed room, situation are fixed with volume, presser, and temperature gas of it. Boyle-Gay lussac to that presser (P), volume (V) and absolute temperature (T) from ideal gas.
p.V= nRT ……. (3.1) p= pressure
V= volume
T= absolute temperature
b. Connection amount mol with
If
n = m/M ………….. (3.2)
or
n = N/Nօ …………. (3.3)
with:
m = massa total gas
M = massa relatif partikel (atom our molekul) gas
Nօ = sum Avogadro
= 6,02 x 1023 partikel/mol
When similarity (3.2) input to similarity (3.1) so will result similarity condition gas next:
pV = n.R.T pV =(m/M).R.T pV = N.K.T
with:
N = amount particle gas
Nօ = sum Avogadro
= 6,02 x 1023 partikel/mol
k = standard Boltzman 1,38 x 10-23 J/k
k = R/Nօ or R= k. Nօ
- Pressure and energy kinetic
If snowen
p = 2 Ēk ( N )
3 V with Ēk = energy kinetic average
- Temperature an flat kinetic energy
Connection temperature and flat kinetic energy can we know with this step
Ēk = 3 k.T
2
- Inside energy
Inside energy is gas definised see like sub kinetic energy all gas particle. If this energy have N some particle of gas in closing tube, so energy in gas V is range of multiplication N with kinetic energy particle Ēk.U = N. Ēk
for monotomik gas
U = 3 N.k.T or U = 3/2 n.R.T
2
for diatomic gas in law temperature ( ± 300 K)
U = 3/2 N.k.T or U = 3/2 n.R.T
for diatomic gas in standard temperature (± 500 K)
U = 5/2 N.k.T or U = 5/2 n.R.T
for diatomic in high temperature (± 1000 K)
U = 7/2 n.K.T or U = 7/2 n.R.T
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