6. gas
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Gas
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Elements that exist as gases at 250C and 1 atmosphere
5.1
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5.1
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• Gas mengikuti bentuk dan volume tempatnya..
• Gas adalah materi yang dapat dimampatkan.• Gas akan tecampur rata seluruhnya apabila berada
dalam satu ruang yang sama.
• Gas memiliki kerapatan yang sangat rendah
dibandingkan dengan cairan dan padatan.
5.1
Ciriciri !isik Gas"
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#atuan $ekanan"
1 pascal %&a' ( 1 )*m2
1 atm ( +,0 mm -g ( +,0 torr
( 101/25 &a
( 1.+ psi
( 2.2 in. -g
5.2arometer
$ekanan(Gaya3uas
%gaya ( massa x percepatan'
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Sea level 1 atm
4 miles 0.5 atm
10 miles 0.2 atm
5.2
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Hukum BoyleHukum BoylePP α 1/Vα 1/VIni berarti tekanan danIni berarti tekanan dan
volume BERBANDINGvolume BERBANDING
TERBALIK aabila milTERBALIK aabila mildan !u"u kon!tan #tidakdan !u"u kon!tan #tidakberuba"$% &onto"n'a( Pberuba"$% &onto"n'a( Pnaik dan V turun%naik dan V turun%
PP11VV11 ) P) P** VV** Robert BoyleRobert Boyle
(1627-1691).(1627-1691).
Son of Earl ofSon of Earl of
or!" #relan$.or!" #relan$.
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Hukum CharlesHukum Charles
Jika tekanan dan molJika tekanan dan molkonstan,maka Vkonstan,maka V α Tα T
V dan TV dan T BERBANDINGBERBANDING
LURUS.LURUS.VV11 V V22
TT11 T T22
! I" one tem#e$at%$e &oes %#, t'eI" one tem#e$at%$e &oes %#, t'e
(ol%me &oes %#)(ol%me &oes %#)
%a&'es arles (1746-%a&'es arles (1746-
1*2+). #solate$ boron1*2+). #solate$ boron
an$ st$ie$ ,ases.an$ st$ie$ ,ases.
Balloonist.Balloonist.
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Gay-Lussac’s LawGay-Lussac’s LawJika mol dan (ol%meJika mol dan (ol%me
konstan,maka *konstan,maka * α Tα T
* dan T* dan T
BERBANDINGBERBANDINGLURUS.LURUS.
**11 * *22
TT11 T T22
I" one tem#e$at%$e &oes %#,I" one tem#e$at%$e &oes %#,
t'e #$ess%$e &oes %#)t'e #$ess%$e &oes %#)
%ose ois /ay-%ose ois /ay-ssa& (177*-1*50)ssa& (177*-1*50)
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Combined Gas Law! T'e &ood ne+s is t'at o% don-t
'a(e to $ememe$ all t'$ee &asla+s) Sin/e t'e a$e all $elated to
ea/' ot'e$, +e /an /omine t'eminto a sin&le e0%ation. BE SUREU 3N4 T5IS E6UATIN)
*1 V1 *2 V2
T1 T2
No, it’s not related to R2D2
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And no+( +e au!e ,or t"i!
-ommer-ial me!!a.e ,rom TP
" so its really not 3#S !in$
of S3
S3 in &emistry stan$s for
Stan$ar$ 3emeratre an$ressre
Stan$ar$ ressre
1 atm (or ane'ivalent)
Stan$ar$
3emeratre 0 $e,
(27+ )
S3 allo8s s to
&omare amonts of,ases bet8een $ifferent
ressres an$
temeratres
S3 allo8s s to
&omare amonts of,ases bet8een $ifferent
ressres an$
temeratres
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-ukum 4vogadro
V α
umlah mol %n'V ( konstan x n
V 1*n1 ( V 2*n2
5./
Constant temperatureConstant pressure
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&ersamaan Gas 6deal
5.
Charles7 la8" V α T %at constant n and P '
4vogadro7s la8" 9 α n %at constant P and T '
oyle7s la8" 9 α %at constant n and T '1
P
V α nT
P
V ( constant x ( R nT
P
nT
P R is the ,as &onstant
PV nRT
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&ada kondisi 0 0C and 1 atm dinamakan stan$ar$
temeratre an$ ressre (S3).
PV = nRT
R =
PV
nT (
%1 atm'%22.13'
%1 mol'%2+/.15 :'
R ( 0.0;205+ 3 • atm * %mol • :'
5.
&ercobaan memperlihatkan bah8a pada #$& 1mol gas ideal memenuhi 22.1 3.
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<ensity %d ' Calculations
d = mV
( P MRT
m is the mass o! the gas in gM is the molar mass o! the gas
=olar =ass %M ' o! a Gaseous #ubstance
dRT
P M ( d is the density o! the gas in g*3
5.
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4 2.103 vessel contains .,5 g o! a gas at 1.00 atm
and 2+.00C. >hat is the molar mass o! the gas?
5./
dRT
P M ( d =
mV
.,5 g
2.10 3( ( 2.21
g
3
M (2.21
g
3
1 atm
x 0.0;21 x /00.15 :3•atm
mol•:
M ( 5., g*mol
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Gas #toichiometry
>hat is the volume o! C@2 produced at /+0 C and 1.00
atm 8hen 5.,0 g o! glucose are used up in the reaction"
C,-12@, %s' A ,@2 %g ' ,C@2 %g ' A ,-2@ %l '
g C,-12@, mol C,-12@, mol C@2 V C@2
5.,0 g C,-12@, 1 mol C,-12@,
1;0 g C,-12@,
x , mol C@2
1 mol C,-12@,
x ( 0.1;+ mol C@2
V (nRT
P
0.1;+ mol x 0.0;21 x /10.15 :3•atm
mol•:
1.00 atm
( ( .+, 3
5.5
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-ukum <alton mengenai $ekanan &arsial
V and T
are&onstant
P 1 P 2 P total = P 1 A P 2
5.,
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Consider a case in 8hich t8o gases 4 and are in a
container o! volume 9.
P 4 ( n AB$V
P (nBB$
V
n 4 is the number o! moles o! 4
n is the number o! moles o!
P $ ( P 4 A P X 4 (n 4
n 4 A n
X (n
n 4 A n
P 4 ( X 4 P $ P ( X P $
P i X i P 3
5.,
mole fraction (X i ) =ni
nT
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4 sample o! natural gas contains ;.2 moles o! C-
0.21 moles o! C2-, and 0.11, moles o! C/-;. 6! the
total pressure o! the gases is 1./+ atm 8hat is the
partial pressure o! propane %C/-;'?
P i ( X i P $
X propane (0.11,
;.2 A 0.21 A 0.11,
P $ ( 1./+ atm
( 0.01/2
P propane ( 0.01/2 x 1./+ atm ( 0.01;1 atm
5.,
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2:Cl@/ %s' 2:Cl %s' A /@2 %g '
Bottle fll of oy,en
,as an$ 8ater vaor
P $ ( P @ A P - @2 2 5.,
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5.,
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emistry in :&tion;
#cuba <iving and the Gas 3a8s
& 9
<epth %!t' &ressure%atm'
0 1
// 2
,, /
5.,
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$eori :inetik =olekul Gas
1. Gas terdiri atas molekulmolekul yang
bergerak random.2. $idak terdapat tarikan maupun tolakan antar
molekul gas.
/. $umbukan antar molekul adalah tumbukanelastik sempurna yakni tidak ada energi
kinetik yang hilang.
. ila dibandingkan dengan volume yangditempati gas volume real molekul gas
dapat diabaikan.
5.+
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&enyimpangan &erilaku 6deal
1 mole o! ideal gas
PV ( nRT
n =PV RT
( 1.0
5.;
Bepulsive orces
4ttractive orces
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E!!ect o! intermolecular !orces on the pressure exerted by a gas.
5.;
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5 ;
PersamaanVan der Waals
Gas )yata
P A %V D nb' ( nRT an2
V 2% ' E
$ekanan
terkoreksi
E
volume
terkoreksi