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‫اﻟﻔﺻل‬
‫اﻻول‬
‫اﻟﺛرﻣوداﯾﻧﻣك‬
( ‫اﻟدرس‬
‫اﻷول‬ )
‫اﻟﺛرﻣوداﯾﻧﻣك‬
‫طرﯾﻘﺔ‬
‫ﻗﺎﻧون‬
‫ھﯾس‬ :
/‫ﺳؤال‬
‫ﻟﻣﺎذا‬
‫ﯾﺗم‬
‫اﻟﻠﺟوء‬
‫إﻟﻰ‬
‫طرﯾﻘﺔ‬
‫ھﯾس‬
‫ﻟﺣﺳﺎب‬
Δ
‫𝐻؟‬𝑟
°
‫ﺟواب‬
/
‫ﱠ‬‫ﻷن‬
‫ﺑﻌض‬
‫اﻟﻣرﻛﺑﺎت‬
‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬
‫ﻻ‬
‫ﯾﻣﻛن‬
‫ﺗﺻﻧﯾﻌﮭﺎ‬
ً‫ة‬‫ﻣﺑﺎﺷر‬
‫ﻣن‬
‫ﻋﻧﺎﺻرھﺎ‬
‫اﻷﺳﺎﺳﯾﺔ‬
‫ﺑﺄﺛﺑت‬
‫ﺻورة‬
(‫)ﻋﻠل‬
‫ﺑﺳﺑب‬
: ‫ﱠ‬‫أن‬
1
(
‫ﺑﻌض‬
‫اﻟﺗﻔﺎﻋﻼت‬
‫ﺗﺳﯾر‬
‫ﺑﺑطء‬
.‫ﺷدﯾد‬
2
(
‫ن‬ ّ‫ﺗﻛو‬
‫ﻣرﻛﺑﺎت‬
‫ﺟﺎﻧﺑﯾﺔ‬
‫ﻏﯾر‬
‫ﻣرﻏوب‬
.‫ﻓﯾﮭﺎ‬
‫ھﯾس؟‬ ‫ﻗﺎﻧون‬ ‫ﻧص‬ ‫ھو‬ ‫ﻣﺎ‬
:‫ﯾﻧص‬
‫)ﻋﻧد‬
‫ﺗﺣوﯾل‬
‫اﻟﻣﺗﻔﺎﻋﻼت‬
‫إﻟﻰ‬
‫ﻧواﺗﺞ‬
‫ﱠ‬‫ﻓﺈن‬
‫اﻟﺗﻐﯾر‬
‫ﻓﻲ‬
‫اﻧﺛﺎﻟﺑﻲ‬
‫اﻟﺗﻔﺎﻋل‬
‫ھو‬
‫ﻧﻔﺳﮫ‬
‫ﺳواء‬
‫ﺗم‬
‫اﻟﺗﻔﺎﻋل‬
‫ﻓﻲ‬
‫ﺧطوة‬
‫واﺣدة‬
.(‫اﻟﺧطوات‬ ‫ﻣن‬ ‫ﺳﻠﺳﻠﺔ‬ ‫ﻋﺑر‬ ‫أو‬
/ ‫ﻣﺛﺎل‬
𝐶‫ﻛﺮاﻓﯿﺖ‬
+ 𝑂2
(𝑔)
⟶𝐶𝑂2
𝑔
( )
∆𝐻𝑟
=− 393. 5 𝐾𝐽/𝑚𝑜𝑙
‫وﻋﻧد‬
‫ﺗﻛوﯾن‬
‫ﺑﺄﻛﺛر‬
‫ﻣن‬
‫ﻣﻌﺎدﻟﺔ‬
‫ﻓﺄن‬
‫ھو‬
‫ﻧﻔﺳﮫ‬ 𝐶𝑂2
∆𝐻𝑟
𝐶‫ﻛﺮاﻓﯿﺖ‬
+
1
2
𝑂2
(𝑔)
⟶𝐶𝑂
𝑔
( )
∆𝐻𝑟
=− 110. 5 𝐾𝐽/𝑚𝑜𝑙
𝐶𝑂
𝑔
( )
+
1
2
𝑂2
(𝑔)
⟶𝐶𝑂2
𝑔
( )
∆𝐻𝑟
=− 283 𝐾𝐽/𝑚𝑜𝑙
𝐶‫ﻛﺮاﻓﯿﺖ‬
+ 𝑂2
(𝑔)
⟶𝐶𝑂2
𝑔
( )
∆𝐻𝑟
=− 393. 5 𝐾𝐽/𝑚𝑜𝑙
‫ھﯾس‬ ‫ﻣﺳﺎﺋل‬ ‫ﺣل‬ ‫ﺣول‬ ‫ﻣﮭﻣﺔ‬ ‫ﻣﻼﺣظﺎت‬
:
1
(
‫ﻋﻧد‬
‫ﻗﻠب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫ﻧﻘﻠب‬
‫إﺷﺎرة‬
‫ﻗﯾﻣﺔ‬
‫اﻻﻧﺛﺎﻟﺑﻲ‬
.
2
(
‫ﻋﻧد‬
‫ﺿرب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫أو‬
‫ﻗﺳﻣﺗﮭﺎ‬
‫ﻋﻠﻰ‬
‫ﻣﻌﺎﻣل‬
‫ﻋددي‬
‫ﻓﺗﺿرب‬
‫أو‬
‫ﺗﻘﺳم‬
‫ﻗﯾﻣﺔ‬
‫اﻻﻧﺛﺎﻟﺑﻲ‬
‫ﺑﻧﻔس‬
.‫اﻟﻌدد‬
3
(
‫ھﻧﺎك‬
‫ﻧوﻋﺎن‬
‫ﻣن‬
:‫اﻟﻣﻌﺎدﻻت‬
:‫اﻷول‬
‫ﻣﻌﺎدﻟﺔ‬
‫اﻟطﻠب‬
(‫)اﻟﮭدف‬
‫وﺗﺳﻣﻰ‬
‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬
،‫اﻟرﺋﯾﺳﯾﺔ‬
:‫واﻟﺛﺎﻧﻲ‬
‫اﻟﻣﻌﺎدﻻت‬
.‫اﻟﻔرﻋﯾﺔ‬
4
(
‫ﻧﻣر‬
‫ﻋﻠﻰ‬
‫ﻣواد‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟرﺋﯾﺳﯾﺔ‬
ً‫ء‬‫اﺑﺗدا‬
‫ﻣن‬
‫أول‬
،‫ﻣﺎدة‬
‫وﻟﯾس‬
ً‫ﺎ‬‫ﺷرط‬
‫أن‬
‫ﻧﻣر‬
‫ﻋﻠﻰ‬
‫ﺟﻣﯾﻊ‬
‫ﻣواد‬
‫ھذه‬
.‫اﻟﻣﻌﺎدﻟﺔ‬
5
(
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟﻔرﻋﯾﺔ‬
‫اﻟﺗﻲ‬
‫ﺗم‬
‫اﻟﺗﻌﺎﻣل‬
‫ﻣﻌﮭﺎ‬
‫ﻻ‬
‫ﯾﺗم‬
‫اﻟرﺟوع‬
‫إﻟﯾﮭﺎ‬
.ً‫ﺛﺎﻧﯾﺔ‬
6
(
‫اﻟﻣﻼﺣظﺔ‬
‫اﻷوﻟﻰ‬
:‫اﻟذھﺑﯾﺔ‬
‫إذا‬
‫ﺗﻛررت‬
‫ﻣﺎدة‬
‫ﻓﻲ‬
‫أﻛﺛر‬
‫ﻣن‬
‫ﻣﻌﺎدﻟﺔ‬
‫ﻓرﻋﯾﺔ‬
‫ﻓﯾﺗم‬
‫ﺗﺟﺎوزھﺎ‬
‫ﻟﻠﻣﺎدة‬
‫اﻟﺗﻲ‬
‫ﺗﻠﯾﮭﺎ‬
‫ﻓﻲ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
.‫اﻟرﺋﯾﺳﯾﺔ‬
7
(
‫اﻟﻣﻼﺣظﺔ‬
:‫اﻟذھﺑﯾﺔ‬
‫إذا‬
‫ﻛﺎﻧت‬
‫اﻟﻣﺎدة‬
‫اﻟﻣﺗﻛررة‬
‫ھﻲ‬
‫آﺧر‬
‫ﻣﺎدة‬
‫ﻓﻲ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟرﺋﯾﺳﯾﺔ‬
‫ﻓﺳﻧﺿطر‬
‫ﻟﻠﺗﻌﺎﻣل‬
‫ﻣﻌﮭﺎ‬
‫ﺑﺷرط‬
.‫اﻟﺗﻐﯾﯾر‬ ‫ﺑﻌد‬ ‫اﻟﻔرﻋﯾﺔ‬ ‫اﻟﻣﻌﺎدﻻت‬ ‫ﻓﻲ‬ ‫ﻣوﻻﺗﮭﺎ‬ ‫ﻋدد‬ ‫ﺣﺳﺎب‬
‫ﻣﺛﺎل‬
1
/
‫اﺣﺳب‬
‫اﻧﺛﺎﻟﺑﻲ‬
‫اﻟﺗﻛوﯾن‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﻟﻠﻣرﻛب‬
‫ﻣن‬
‫ﻋﻧﺎﺻره‬
‫اﻷﺳﺎﺳﯾﺔ‬
‫ﺑﺄﺛﺑت‬
:‫ﺻورھﺎ‬ 𝐶𝑆2
(𝐿)
Δ = ?
𝐶‫ﻛﺮاﻓﯿﺖ‬
+ 2𝑆‫ﻣﻌﯿﻨﻲ‬
→ 𝐶𝑆2
(𝐿)
𝐻𝑓
°
:‫اﻵﺗﯾﺔ‬ ‫اﻟﺣرارﯾﺔ‬ ‫اﻟﻣﻌﺎدﻻت‬ ‫أﻋطﯾت‬ ‫إذا‬
= - 394 KJ/mol
1
( )𝐶‫ﻛﺮاﻓﯿﺖ‬
+ 𝑂2
𝑔
( )
→𝐶𝑂2
(𝑔)
∆𝐻𝑟
°
= - 296 KJ/mol
(2) 𝑆‫ﻣﻌﯿﻨﻲ‬
+ 𝑂2
𝑔
( )
→𝑆𝑂2
(𝑔)
∆𝐻𝑟
°
= - 1072 KJ/mol
3
( )𝐶𝑆2
(𝐿)
+ 3𝑂2
(𝑔)
→ 𝐶𝑂2
(𝑔)
+ 2𝑆𝑂2
(𝑔)
∆𝐻𝑟
°
/‫اﻟﺣل‬
‫ﺗﺑﻘﻰ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
1
(
‫ﻛﻣﺎ‬
،‫ھﻲ‬
‫وﻧﺿرب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
2
(
×
2
،
‫وﺗﻘﻠب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
3
(
:
= - 394
(1) 𝐶‫ﻛﺮاﻓﯿﺖ‬
+ 𝑂2
→ 𝐶𝑂2
∆𝐻𝑟
°
KJ/mol
= - 592
(2)2𝑆 + 2𝑂2
→ 2𝑆𝑂2
∆𝐻𝑟
°
KJ/mol
= + 1072 KJ/mol
3
( )𝐶𝑂2
(𝑔)
+ 2𝑆𝑂2
(𝑔)
→ 𝐶𝑆2
(𝐿)
+ 3𝑂2
(𝑔)
∆𝐻𝑟
°
Δ = = 86 KJ/mol
𝐶 ‫ﻛﺮاﻓﯿﺖ‬
+ 𝑆‫ﻣﻌﯿﻨﻲ‬
→ 𝐶𝑆2
(𝐿)
𝐻𝑓
°
∆𝐻𝑟
°
‫اﻻول‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
‫ﯾﺗم‬
‫اﻟﻠﺟوء‬
‫إﻟﻰ‬
‫طرﯾﻘﺔ‬
‫ھﯾس‬
‫ﻟﺣﺳﺎب‬
Δ
‫ﱠ‬‫ﻷن‬
‫ﺑﻌض‬
‫اﻟﻣرﻛﺑﺎت‬
‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬
‫ﯾﻣﻛن‬
‫ﺗﺻﻧﯾﻌﮭﺎ‬ 𝐻𝑟
°
‫ﺻورة‬ ‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﻋﻧﺎﺻرھﺎ‬ ‫ﻣن‬ ً‫ة‬‫ﻣﺑﺎﺷر‬
)
T, F
(
‫اﻟﺟواب‬
/
F
2
.
:‫اﻟﻣﻌﺎدﻻت‬ ‫ﻣن‬ ‫ﻧوﻋﺎن‬ ‫ھﻧﺎك‬
)
A
:‫اﻷول‬
‫ﻣﻌﺎدﻟﺔ‬
‫اﻟطﻠب‬
(‫)اﻟﮭدف‬
‫وﺗﺳﻣﻰ‬
‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬
،‫اﻟرﺋﯾﺳﯾﺔ‬
:‫اﻟﺛﺎﻧﻲ‬
‫اﻟﻣﻌﺎدﻻت‬
.‫اﻟﻔرﻋﯾﺔ‬
)
B
:‫اﻷول‬
‫ﻣﻌﺎدﻟﺔ‬
‫اﻟطﻠب‬
(‫)اﻟﮭدف‬
‫وﺗﺳﻣﻰ‬
‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬
،‫اﻟرﺋﯾﺳﯾﺔ‬
:‫اﻟﺛﺎﻧﻲ‬
‫اﻟﻣﻌﺎدﻻت‬
.‫اﻟرﺋﯾﺳﯾﺔ‬
‫اﻟﺟواب‬
/
A
3
.
‫اﻟﻣﻼﺣظﺔ‬
‫اﻷوﻟﻰ‬
:‫اﻟذھﺑﯾﺔ‬
‫اذا‬
‫وﺟدت‬
‫ﻣﺎدة‬
‫ﻓﻲ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟرﺋﯾﺳﯾﺔ‬
‫وھﻲ‬
‫ﻣﺗﻛررة‬
‫ﻓﻲ‬
‫اﻛﺛر‬
‫ﻣن‬
‫اﻟﺗﻲ‬ ‫اﻟﻣﺎدة‬ ‫اﻟﻰ‬ ‫اﻟﻣﺎدة‬ ‫ھذه‬ ‫ﺗﺟﺎوز‬ ‫ﻓﯾﺗم‬ ‫ﻓرﻋﯾﺔ‬ ‫ﻣﻌﺎدﻟﺔ‬
‫اﻟرﺋﯾﺳﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﻓﻲ‬ ‫ﺗﻠﯾﮭﺎ‬
)
T, F
(
‫اﻟﺟواب‬
/
T
( ‫اﻟدرس‬
‫اﻟﺛﺎﻧﻲ‬ )
‫ﺣﺳﺎﺑﺎت‬
‫ﺑﺎﺳﺗﺧدام‬
‫ﻗﺎﻧون‬
‫ھﯾس‬
‫س‬
1
/
‫إذا‬
‫أﻋطﯾت‬
‫اﻟﻣﻌﺎدﻻت‬
‫اﻟﺣرارﯾﺔ‬
‫اﻵﺗﯾﺔ‬
‫ﻋﻧد‬
‫اﻟظروف‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
)
STP
:(
Δ = 25 KJ
1
( )𝐹𝑒𝑂(𝑠)
+ 𝐻2
(𝑔)
→ 𝐹𝑒(𝑠)
+ 𝐻2
𝑂(𝑔)
𝐻𝑟
°
Δ = 318 KJ
2
( )3𝐹𝑒𝑂(𝑠)
+
1
2
𝑂2
(𝑔)
→ 𝐹𝑒3
𝑂4
(𝑠)
𝐻𝑟
°
Δ = - 242 KJ
3
( )𝐻2
(𝑔)
+
1
2
𝑂2
(𝑔)
→ 𝐻2
𝑂(𝑔)
𝐻𝑟
°
‫اﺣﺳب‬
Δ
‫ﻟﻠﺗﻔﺎﻋل‬
:‫اﻟﺗﺎﻟﻲ‬ 𝐻𝑟
°
Δ =?
3𝐹𝑒(𝑠)
+ 4𝐻2
(𝑔)
→ 𝐹𝑒3
𝑂4
(𝑠)
+ 4𝐻2
(𝑔)
𝐻𝑟
°
/‫اﻟﺣل‬
‫ﻧﻘﻠب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
1
(
‫وﻧﺿرﺑﮭﺎ‬
×
3
‫وﺗﺑﻘﻰ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
2
(
‫ﻛﻣﺎ‬
‫ھﻲ‬
‫وﻧﻘﻠب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
3
:(
= -75KJ
1
( ) 3𝐹𝑒 𝑠
( )
+ 3𝐻2
𝑂 ⟶3𝐹𝑒𝑂 𝑠
( )
+ 3𝐻2
∆𝐻𝑟
°
2
( )𝐹𝑒𝑂 𝑆
( )
+
1
2
𝑂2
⟶𝐹𝑒3
𝑂4
𝑆
( )
∆𝐻𝑟
°
= − 318𝐾𝐽
3
( )𝐻2
𝑂
𝑔
( )
⟶𝐻2
𝑔
( )
+
1
2
𝑂2(𝑔)
∆𝐻𝑟
°
= + 242𝐾𝐽
Δ
=
-
151
KJ2 3𝐹𝑒(𝑠)
+ 4𝐻2
𝑂(𝑔)
→ 𝐹𝑒3
𝑂4
+ 4𝐻
𝐻𝑟
°
/‫ﻣﻼﺣظﺔ‬
‫ھﻧﺎ‬
‫ﻧطﺑق‬
‫اﻟﻣﻼﺣظﺔ‬
‫اﻟذھﺑﯾﺔ‬
‫اﻷوﻟﻰ‬
‫ﺑﻌدم‬
‫ﻣوازﻧﺔ‬
‫ﮫ‬‫ﱠ‬‫ﻧ‬‫ﻷ‬
‫ﻣﺗﻛرر‬
‫أﻛﺛر‬
‫ﻣن‬
‫ﻣرة‬
‫ﻓﻲ‬
‫اﻟﻣﻌﺎدﻻت‬
،‫اﻟﻔرﻋﯾﺔ‬ 𝐻2
𝑂
‫وﻛذﻟك‬
‫ﻧطﺑق‬
‫اﻟﻣﻼﺣظﺔ‬
‫اﻟذھﺑﯾﺔ‬
‫اﻟﺛﺎﻧﯾﺔ‬
‫ﺑﺿرورة‬
‫ﻣوازﻧﺔ‬
‫رﻏم‬
‫ﺗﻛراره‬
‫وﻟﻛن‬
‫ﺑﻌد‬
‫ﺣﺳﺎب‬
‫ﻣوﻻﺗﮫ‬
‫اﻟﺳﺎﺑﻘﺔ‬
‫ﺑﻌد‬ 𝐻2
‫اﻟﺗﻐﯾﯾر‬
.
‫س‬
2
/
‫إذا‬
‫ﻋﻠﻣت‬
‫ﱠ‬‫أن‬
‫اﻧﺛﺎﻟﺑﻲ‬
‫اﺣﺗراق‬
ّ‫ل‬‫ﻛ‬
‫ﻣن‬
‫ﻏﺎز‬
CO
‫و‬
‫و‬
‫ﺑوﺣدات‬
KJ/mol
‫ھﻲ‬
‫ﻋﻠﻰ‬
:‫اﻟﺗواﻟﻲ‬
-) 𝐻2
𝐶𝐻3
𝑂𝐻
727
-/
286
-/
284
،(
‫اﺣﺳب‬
Δ
‫ﺑﺎﺳﺗﺧدام‬
‫ﻗﺎﻧون‬
‫ھﯾس‬
‫ﻟﻠﺗﻔﺎﻋل‬
:‫اﻵﺗﻲ‬ 𝐻𝑟
°
𝐶𝑂 + 2𝐻2
→ 𝐶𝐻3
𝑂𝐻
.‫ﺑﺎﻟﺳؤال‬ ‫ﺗﻌط‬ ‫ﻟم‬ ‫إذا‬ ‫اﻟﻔرﻋﯾﺔ‬ ‫اﻻﺣﺗراق‬ ‫ﻣﻌﺎدﻻت‬ ‫ﻧﻛﺗب‬ ‫ﻣن‬ ‫ﻧﺣن‬
‫ﺑطرﯾﻘﺔ‬ ‫ﻧﺣﻠﮫ‬ ‫أن‬ ‫ﯾﻣﻛن‬ ‫ﱠ‬‫ﻷن‬ ،‫ھﯾس‬ ‫ﺑطرﯾﻘﺔ‬ ‫اﻟﺳؤال‬ ‫ﺣددﻧﺎ‬
.(‫)اﻟﺳﻣﯾﺷن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻟﺗﻛوﯾن‬ ‫اﻧﺛﺎﻟﺑﻲ‬
= - 284 KJ/mol
(1) 𝐶𝑂 +
1
2
𝑂2
→ 𝐶𝑂2
∆𝐻𝑟
°
= - 286 KJ/mol
2
( )𝐻2
+
1
2
𝑂2
→ 𝐻2
𝑂 ∆𝐻𝑟
°
= - 727 KJ/mol
3
( )𝐶𝐻3
𝑂𝐻 +
3
2
𝑂2
→ 𝐶𝑂2
+ 2𝐻2
𝑂 ∆𝐻𝑟
°
‫وﻟﻠﺣﺻول‬
‫ﻋﻠﻰ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
،‫اﻟرﺋﯾﺳﯾﺔ‬
‫ﺗﺑﻘﻰ‬
‫اﻟﻣﻌﺎدﻟﺔ‬
)
1
(
‫ﻛﻣﺎ‬
،‫ھﻲ‬
‫وﻧﺿرب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟﻔرﻋﯾﺔ‬
)
2
(
2
×
،
‫وﻧﻘﻠب‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟﻔرﻋﯾﺔ‬
)
3
:(
= - 284 KJ/mol
(1) 𝐶𝑂 +
1
2
𝑂2
→ 𝐶𝑂2
∆𝐻𝑟
°
= - 572 KJ/mol
2
( )2𝐻2
+ 𝑂2
→ 2𝐻2
𝑂 ∆𝐻𝑟
°
= + 727 KJ/mol
3
( )𝐶𝑂2
+ 2𝐻2
𝑂 → 𝐶𝐻3
𝑂𝐻 +
3
2
𝑂2
∆𝐻𝑟
°
Δ = - 129 KJ/mol
𝐶𝑂 + 2𝐻2
→ 𝐶𝐻3
𝑂𝐻 𝐻𝑟
°
/‫ﻣﻼﺣظﺔ‬
‫ﯾﻣﻛن‬
‫ﺣل‬
‫اﻟﺳؤال‬
‫ﺑطرﯾﻘﺔ‬
‫اﻧﺛﺎﻟﺑﻲ‬
‫اﻟﺗﻛوﯾن‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
)
Σ
(
‫ﺑﻌد‬
‫أن‬
‫ﻧﺣول‬
‫ﻗﯾﻣﺔ‬
‫اﻻﻧﺛﺎﻟﺑﻲ‬
‫ﻟﻠﻣﯾﺛﺎﻧول‬
‫ﻣن‬
‫اﻹﺷﺎرة‬ ‫ﺑﻘﻠب‬ ‫وذﻟك‬ (‫)اﻟﻣﺎص‬ ‫اﻟﺗﻛوﯾن‬ ‫إﻟﻰ‬ (‫)اﻟﺑﺎﻋث‬ ‫اﻻﺣﺗراق‬
‫ﻟﻠﻣوﺟب‬ ‫اﻟﺳﺎﻟب‬ ‫ﻣن‬
.
‫س‬
3
/
‫اﺣﺳب‬
‫اﻧﺛﺎﻟﺑﻲ‬
‫اﻟﺗﻛوﯾن‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
(
)𝐻𝑃𝑂3
= - 180KJ
𝑃4
𝑂10
+ 4𝐻𝑁𝑂3
→4𝐻𝑃𝑂3
+ 2𝑁2
𝑂5
∆𝐻𝑟
°
‫ﻋﻠﻣت‬ ‫اذا‬
Δ
=
-)
2984
(
KJ/mol 𝐻𝑓 𝑃4
𝑂10
°
Δ
=
-)
174
(
KJ/mol 𝐻𝑓 𝐻𝑁𝑂3
°
Δ =(-43)KJ/mol ??
𝐻𝑓 𝑁2
𝑂5
°
Δ𝐻𝑟
°
= ∑ 𝑛∆ 𝐻𝑓(𝑃)
°
− ∑ 𝑛 ∆𝐻𝑓 𝑅
( )
°
Δ𝐻𝑟
°
= [4Δ𝐻𝑓(𝐻𝑃𝑂3
)
°
+ 2Δ𝐻𝑓(𝑁2
𝑂5
)
°
] − [Δ𝐻𝑓(𝑃4
𝑂10
)
°
+ 4 Δ𝐻𝑓(𝐻𝑁𝑂3
)
°
]
− 180 = 4Δ𝐻𝑓 𝐻𝑃𝑂3
( )
°
+ 2 − 43
( )
⎡
⎢
⎣
⎤
⎥
⎦
− − 2984
( ) + 4 − 174
( )
[ ]
− 180 = 4Δ𝐻𝑓 𝐻𝑃𝑂3
( )
°
− 86
⎡
⎢
⎣
⎤
⎥
⎦
− (− 3680)]
- 4∆𝐻𝑓 𝐻𝑃𝑂3
( )
°
= 3594 + 180⟹4∆𝐻𝑓 𝐻𝑃𝑂3
( )
°
=− 3594 − 180
∴∆𝐻𝑓 𝐻𝑃𝑂3
( )
°
=
−3774
4
⟹∆𝐻𝑓 𝐻𝑃𝑂3
( )
°
=− 943. 5 𝐾𝐽/𝑚𝑜𝑙
(‫اﻟﺛﺎﻟث‬ ‫)اﻟدرس‬
‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬
: ‫اﻹﻧﺗروﺑﻲ‬
‫»ھﻲ‬
‫داﻟﺔ‬
‫ﺣﺎﻟﺔ‬
‫ﺛرﻣوداﯾﻧﻣﯾﻛﯾﺔ‬
‫ﺗﻌﺗﺑر‬
‫ﻣﻘﯾﺎس‬
‫ﻟدرﺟﺔ‬
،‫اﻟﻌﺷواﺋﯾﺔ‬
‫أو‬
‫ﻻ‬
‫اﻧﺗظﺎم‬
،‫اﻟﻧظﺎم‬
‫وﯾرﻣز‬
‫ﻟﮭﺎ‬
)
S
،(
‫وﺗﻘﺎس‬
‫ﺑوﺣدة‬
)
J/K mol
.«(
‫اﻻﻧﺗروﺑﻲ؟‬ ‫اﻟﺣﺎﻟﺔ‬ ‫داﻟﺔ‬ ‫ﻓﺎﺋدة‬ ‫ﻣﺎ‬
/‫ج‬
‫ﯾﺳﺗﻔﺎد‬
‫ﻣﻧﮭﺎ‬
‫ﻟﻠﺗﻧﺑؤ‬
‫ﺑﺗﻠﻘﺎﺋﯾﺔ‬
،‫اﻟﺗﻔﺎﻋل‬
‫ﻓﻛﻠﻣﺎ‬
‫ﻛﺎن‬
‫اﻟﻼﻧظﺎم‬
ً‫ﻼ‬‫ﻗﻠﯾ‬
‫)اﻟﻌﺷواﺋﯾﺔ‬
(‫أﻛﺑر‬
‫ﻛﺎﻧت‬
‫ﻗﯾﻣﺔ‬
‫أﻛﺑر‬ ‫اﻻﻧﺗروﺑﻲ‬
)
ΔS
=
(+
‫واﻟﻌﻛس‬
‫ﺻﺣﯾﺢ‬
:‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻻﻧﺗروﺑﻲ‬ ‫ﺣﺳﺎب‬
∆𝑆𝑟
о
= ∑𝑛 𝑆(𝑃)
о
− ∑𝑛 𝑆(𝑅)
о
‫طﺎﻗﺔ‬
‫ﻛﺑس‬
‫اﻟﺣرة‬
)
ΔG
:(
‫وﯾﻣﻛن‬
‫ﺣﺳﺎب‬
‫اﻟطﺎﻗﺔ‬
‫اﻟﺣرة‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﻟﻠﺗﻔﺎﻋل‬
‫ﺑﺎﻻﻋﺗﻣﺎد‬
‫ﻋﻠﻰ‬
‫اﻟطﺎﻗﺔ‬
‫اﻟﺣرة‬
‫ﻟﻠﺗﻛوﯾن‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﻣن‬
‫ﺧﻼل‬
‫اﺳﺗﺧدام‬ ∆𝐺𝑓
°
(‫)اﻟﺳﻣﯾﺷن‬ ‫اﻟﻣﺟﻣوع‬ ‫ﻗﺎﻧون‬
Δ
=𝐺𝑟
°
∑ 𝑛 ∆𝐺𝑓(𝑃)
°
− ∑ 𝑛 ∆𝐺𝑓(𝑅)
°
:‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬
‫ﻟﻧﺎ‬ ‫ﺗﺗﯾﺢ‬ ‫ﺛرﻣوداﯾﻧﻣﯾﻛﯾﺔ‬ ‫ﺣﺎﻟﺔ‬ ‫داﻟﺔ‬ ‫»ھﻲ‬
‫اﻟﺗﻲ‬ ‫اﻟﻌظﻣﻰ‬ ‫اﻟطﺎﻗﺔ‬ ‫ﺗﻣﺛل‬ ‫وھﻲ‬ ،‫اﻟﺗﻔﺎﻋل‬ ‫ﺑﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺗﻧﺑؤ‬
‫ﯾﻣﻛن‬
،‫واﻻﻧﺗروﺑﻲ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﻓﻲ‬ ‫اﻟﺗﻐﯾر‬ ‫ﻗﯾﺎس‬ ‫ﻣن‬ ‫ﻋﻠﯾﮭﺎ‬ ‫اﻟﺣﺻول‬
‫اﻟﺗﺎﻟﯾﺔ‬ ‫اﻟﻌﻼﻗﺔ‬ ‫ﺑﺣﺳب‬
:
∆𝐺
о
= ∆𝐻
о
− 𝑇∆𝑆
о
ΔG
=
‫ﺳﺎﻟﺑﺔ‬
‫)اﻟﺗﻔﺎﻋل‬
‫أو‬
‫اﻟﺗﻐﯾر‬
‫اﻟﻔﯾزﯾﺎﺋﻲ‬
.(‫ﺗﻠﻘﺎﺋﻲ‬
ΔG
=
‫ﻣوﺟﺑﺔ‬
‫)اﻟﺗﻔﺎﻋل‬
‫أو‬
‫اﻟﺗﻐﯾر‬
‫اﻟﻔﯾزﯾﺎﺋﻲ‬
‫ﻏﯾر‬
‫ﺗﻠﻘﺎﺋﻲ‬
)
ΔG
=
‫ﺻﻔر‬
‫)اﻟﺗﻔﺎﻋل‬
‫أو‬
‫اﻟﺗﻐﯾر‬
‫اﻟﻔﯾزﯾﺎﺋﻲ‬
‫ﻓﻲ‬
‫ﺣﺎﻟﺔ‬
.(‫اﺗزان‬
‫ﻣﻼﺣظﺎت‬
‫ﻣﮭﻣﺔ‬ :
1
.
Δ
‫ﻟﻠﻌﻧﺎﺻر‬
‫اﻟﺣرة‬
‫ﺑﺄﺛﺑت‬
‫ﺻورھﺎ‬
=
.‫ﺻﻔر‬ 𝐻𝑓
°
‫ﻣﺛﺎل‬
/
/
/
/
:(
...
‫اﻟﺦ‬
.( 𝐴𝑙(𝑠)
𝐶𝑙2
(𝑔)
𝑁2
(𝑔)
𝑂2
(𝑔)
𝐻2
(𝑔)
2
.
‫أﻓﺿل‬
‫طرﯾﻘﺔ‬
‫ﻻﺳﺗﺧدام‬
‫اﻟﺳﻣﯾﺷن‬
‫ھو‬
‫إﻧﮭﺎء‬
‫ﻧﺎﺗﺞ‬
ّ‫ل‬‫ﻛ‬
‫طرف‬
‫ﺑدﻗﺔ‬
‫ﺛم‬
‫ﻧﻘوم‬
‫ﺑﻌﻣﻠﯾﺔ‬
‫طرح‬
‫اﻟطرف‬
‫اﻷول‬
‫ﻣن‬
.‫اﻟﺛﺎﻧﻲ‬
3
.
‫رﺑﻣﺎ‬
‫ﺗﻛون‬
Δ
‫ﻣﻌﻠوﻣﺔ‬
‫و‬
Δ
‫ﻟﻣﻌظم‬
‫ﻣواد‬
‫اﻟﻣﻌﺎدﻟﺔ‬
‫ﻣﻌﻠوﻣﺔ‬
‫وﯾﻛون‬
‫اﻟﻣطﻠوب‬
Δ
‫ﻟﻣﺎدة‬
‫ﻣﺟﮭوﻟﺔ‬
.‫واﺣدة‬ 𝐺𝑟
°
𝐺𝑓
°
𝐺𝑓
°
4
.
‫إذا‬
‫ﻛﺎن‬
‫اﻟطرف‬
‫اﻟﺛﺎﻧﻲ‬
‫ﻧﺎﺗﺟﮫ‬
‫ﺳﺎﻟب‬
‫ﻓﺗﺻﺑﺢ‬
‫اﻟﻌﻣﻠﯾﺔ‬
:‫اﻟﺣﺳﺎﺑﯾﺔ‬
‫اﻟﺛﺎﻧﻲ‬ ‫اﻟطرف‬ + ‫اﻷول‬ ‫اﻟطرف‬
‫س‬
1
/
‫ﻋرف‬
‫طﺎﻗﺔ‬
‫ﻛﺑس‬
‫اﻟﺣرة‬
‫ﻟﻠﺗﻛوﯾن‬
،‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫وﻣﺎ‬
‫ھﻲ‬
‫وﺣداﺗﮭﺎ؟‬
»/ ‫اﻟﺟواب‬
‫ﺗﻛوﯾن‬ ‫ﻋﻧد‬ ‫اﻟﺣرة‬ ‫اﻟطﺎﻗﺔ‬ ‫ﻓﻲ‬ ‫اﻟﺗﻐﯾﯾر‬ ‫ﻣﻘدار‬ ‫ھﻲ‬
‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﻋﻧﺎﺻرھﺎ‬ ‫ﻣن‬ ‫ﻣرﻛب‬ ‫أي‬ ‫ﻣن‬ ‫واﺣد‬ ‫ﻣول‬
،‫ﺻورة‬
‫وﻋﻧد‬
‫اﻟظروف‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
)
1
atm/25
(
‫وﯾرﻣز‬
‫ﻟﮭﺎ‬
)
(
‫ووﺣداﺗﮭﺎ‬
)
KJ/mol)» s ℃
𝐷𝐺𝑓
°
‫ﻣﺛﺎل‬
2
/
‫اﺣﺳب‬
‫طﺎﻗﺔ‬
‫ﻛﺑس‬
‫اﻟﺣرة‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﻟﻠﺗﻔﺎﻋل‬
‫اﻟﺗﺎﻟﻲ‬
‫ﻋﻧد‬
‫اﻟظروف‬
،‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﺛم‬
‫ن‬ّ‫ﯾ‬‫ﺑ‬
‫ھل‬
‫ﯾﺟري‬
‫اﻟﺗﻔﺎﻋل‬
ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬
‫أم‬
:‫اﻟظروف‬ ‫ھذه‬ ‫ﻋﻧد‬ ،‫ﻻ‬
2𝐶6
𝐻6
(𝐿)
+ 15𝑂2
(𝑔)
→ 12𝐶𝑂2
(𝑔)
+ 6𝐻2
𝑂(𝐿)
:‫ﻋﻠﻣت‬ ‫إذا‬
= (- 394) KJ/mol,
∆𝐺𝑓𝐶𝑂2
°
= (- 237) KJ/mol
∆𝐺𝑓𝐻2
𝑂
°
= (173) KJ/mol
∆𝐺𝑓𝐶6
𝐻6
°
/‫اﻟﺣل‬
Δ
= 𝐺𝑟
°
∑ 𝑛 ∆𝐺𝑓(𝑃)
°
− ∑ 𝑛 ∆𝐺𝑓(𝑅)
°
Δ
=
]
12
+
6
[
-
]
+
15
[ 𝐺𝑟
°
∆𝐺𝑓𝐶𝑂2
°
∆𝐺𝑓𝐻2
𝑂
°
2∆𝐺𝑓𝐶6
𝐻6
°
∆𝐺𝑓𝑂2
°
= Δ = [(- 4728) + (- 1422)] - (346)
𝐺𝑟
°
Δ = - 6496 KJ/mol = ‫)ﺳﺎﻟﺒﺔ‬ , ( ‫اﻟﺘﻔﺎﻋﻞ‬
‫ﺗﻠﻘﺎﺋﻲ‬
‫ﱠ‬‫ﻷن‬
∴ 𝐺𝑟
°
∆𝐺°𝑟
‫ﺗﻣرﯾن‬
1
/
‫اﺣﺳب‬
‫طﺎﻗﺔ‬
‫ﻛﺑس‬
‫اﻟﺣرة‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ﻟﻠﺗﻔﺎﻋل‬
‫اﻟﺗﺎﻟﻲ‬
‫ﻋﻧد‬
‫اﻟظروف‬
،‫اﻟﻘﯾﺎﺳﯾﺔ‬
‫ن‬ّ‫ﯾ‬‫وﺑ‬
‫ھل‬
‫ﯾﺟري‬
‫اﻟﺗﻔﺎﻋل‬
ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬
‫أم‬
‫ﻻ؟‬
2𝑁𝑂(𝑔)
+ 𝑂2
(𝑔)
→2𝑁𝑂2
(𝑔)
:‫ﻋﻠﻣت‬ ‫إذا‬
∆𝐺𝑓𝑁𝑂
°
= 87
𝐾𝐽
𝑚𝑜𝑙
∆𝐺𝑓𝑁𝑂2
°
= 52
𝐾𝐽
𝑚𝑜𝑙
/‫اﻟﺣل‬
Δ
=
]
2
)
[(
-
]
2
)
(
+
[ 𝐺𝑟
°
∆𝐺𝑓𝑁𝑂2
°
∆𝐺𝑓𝑁𝑂
°
∆𝐺𝑓𝑂2
°
=
]
2
)
52
[(
-
]
2
)
87
(
+
0
[
Δ = (104) - (174) ⇒ Δ = - 70 KJ/mol ‫ﺗﻠﻘﺎﺋﻲ‬
∴ 𝐺𝑟
°
𝐺𝑟
°
‫ﻣﻼﺣظﺔ‬
/
‫ﻟﻠﻌﻨﺎﺻﺮ‬
‫اﻟﺤﺮة‬
‫ﺑﺎﺛﺒﺖ‬
‫ﺻﻮرة‬
=
‫ﺻﻔﺮ‬ ∆𝐺
°
‫اﻟﺛﺎﻟث‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
Δ
‫ﻟﻠﻌﻧﺎﺻر‬
‫اﻟﺣرة‬
‫ﺑﺄﺛﺑت‬
‫ﺻورھﺎ‬
=
.‫ﺻﻔر‬ 𝐺𝑓
°
)
T, F
(
‫اﻟﺟواب‬
/
T
2
.
‫أﻓﺿل‬
‫طرﯾﻘﺔ‬
‫ﻻﺳﺗﺧدام‬
‫اﻟﺳﻣﯾﺷن‬
‫ھو‬
‫إﻧﮭﺎء‬
‫ﻧﺎﺗﺞ‬
ّ‫ل‬‫ﻛ‬
‫طرف‬
‫ﺑدﻗﺔ‬
‫ﺛم‬
‫ﻧﻘوم‬
‫ﺑﻌﻣﻠﯾﺔ‬
‫ﺟﻣﻊ‬
.‫اﻟﺛﺎﻧﻲ‬ ‫ﻣن‬ ‫اﻷول‬ ‫اﻟطرف‬
)
T, F
(
‫اﻟﺟواب‬
/
F
3
.
‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﺗﻛوﯾن‬ ‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬
:
)
A
‫ھﻲ‬
‫ﻣﻘدار‬
‫اﻟﺗﻐﯾﯾر‬
‫ﻓﻲ‬
‫اﻟطﺎﻗﺔ‬
‫اﻟﺣرة‬
‫ﻋﻧد‬
‫ﺗﻛوﯾن‬
‫ﻣول‬
‫واﺣد‬
‫ﻣن‬
‫أي‬
‫ﻣرﻛب‬
‫ﻣن‬
‫ﻋﻧﺎﺻرھﺎ‬
،‫ﺻورة‬ ‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬
)
B
‫اﻟظروف‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
)
1
atm/50
(
‫وﯾرﻣز‬
‫ﻟﮭﺎ‬
)
(
‫ووﺣداﺗﮭﺎ‬
)
KJ/mol
.( ∆𝐺𝑓
°
)
C
‫اﻟظروف‬
‫اﻟﻘﯾﺎﺳﯾﺔ‬
)
1
atm/25
(
‫وﯾرﻣز‬
‫ﻟﮭﺎ‬
)
(
‫ووﺣداﺗﮭﺎ‬
)
KJ/mol
.( ∆𝐺𝑓
°
‫اﻟﺟواب‬
/
A & C
( ‫اﻟراﺑﻊ‬ ‫)اﻟدرس‬
‫اﻟﺗﻔﺎﻋﻼت‬ ‫ﺳﯾر‬ ‫وﺗﺟﺎه‬ ‫ﻛﺑس‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬
‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬
‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬ ‫اﻟﺗﻔﺎﻋﻼت‬ ‫ﺳﯾر‬ ‫واﺗﺟﺎه‬ ‫ﻛﺑس‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬
∆𝐺𝑟
° = ∆𝐻𝑟
° − 𝑇∆𝑆𝑟
‫ﺳؤال‬
/
‫اﻟﺗﻔﺎﻋل؟‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫ﯾﺿﻣﻧﺎن‬ ‫ﻋﺎﻣﻠﯾن‬ ‫أﻛﺛر‬ ‫ھﻣﺎ‬ ‫ﻣﺎ‬
/‫ج‬
‫ﱠ‬‫إن‬
‫اﻟﺘﻐﯿﺮ‬
‫ﻓﻲ‬
‫اﻟﻄﺎﻗﺔ‬
‫اﻟﺤﺮة‬
)
Δ
(
‫ﯾﺘﻀﻤﻦ‬
‫ﻋﺎﻣﻠﯿﻦ‬
‫ﻣﮭﻤﯿﻦ‬
‫ﯾﺆﺛﺮان‬
‫ﻋﻠﻰ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
،‫اﻟﺘﻔﺎﻋﻞ‬
:‫وھﻤﺎ‬ 𝐺𝑟
°
1
.
𝐷𝐻𝑟
о
2
.
𝐷𝑆𝑟
°
‫واذا‬
‫ﻛﺎﻧﺖ‬
‫اﺷﺎرة‬
‫و‬
‫ﻣﺘﺸﺎﺑﮭﺔ‬
‫ﺗﻜﻮن‬
‫درﺟﺔ‬
‫اﻟﺤﺮارة‬
‫ھﻲ‬
‫اﻟﻤﺘﺤﻜﻢ‬
‫اﻟﺮﺋﯿﺴﻲ‬
‫ﻓﻲ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
‫اﻟﺘﻔﺎﻋﻞ‬ 𝐷𝐻𝑟
о
𝐷𝑆𝑟
о
/‫ﻋﻠل‬
‫ﺗﻠﻘﺎﺋﯾﺔ؟‬ ‫أﻛﺛر‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻛﺎن‬ ‫ﻋﺎﻟﯾﺔ‬ ‫اﻻﻧﺗروﺑﻲ‬ ‫ﻛﺎﻧت‬ ‫ﻛﻠﻣﺎ‬
/‫ج‬
(∆𝐺°𝑟
= ∆𝐻°𝑟
− 𝑇∆𝑆°𝑟
)
‫ﱠ‬‫ﻷن‬
‫اﻻﻧﺘﺮوﺑﻲ‬
‫ﺗﻘﻊ‬
‫ﺿﻤﻦ‬
‫اﻟﺤﺪ‬
)
‫اﻟﺴﺎﻟﺐ‬
‫وﺑﺎﻟﺘﺎﻟﻲ‬
‫ﻛﻠﻤﺎ‬
‫ﺗﻜﻮن‬
‫ﻗﯿﻤﺔ‬
‫ھﺬا‬
‫اﻟﺤﺪ‬
‫أﻋﻠﻰ‬
‫ﻣﻦ‬
)
> 𝑇∆𝑆°𝑟
)
∆𝐻°𝑟
∆𝐻°𝑟
(
‫ﻛﺎﻧﺖ‬
‫ﻗﯿﻤﺔ‬
=
،‫ﺳﺎﻟﺒﺔ‬
‫وﺑﺎﻟﺘﺎﻟﻲ‬
‫ﯾﻜﻮن‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﺗﻠﻘﺎﺋﻲ‬
. 𝑇∆𝑆°𝑟
𝐷𝐺°𝑟
‫ﻣﻼﺣظﺔ‬
/
‫ﺣﯿﻨﻤﺎ‬
‫ﺗﻜﻮن‬
‫إﺷﺎرات‬
)
ΔH, ΔS
(
‫ﻣﺨﺘﻠﻔﺔ‬
‫ﻓﻠﯿﺲ‬
‫ھﻨﺎك‬
‫ﺗﺄﺛﯿﺮ‬
‫ﻟﺪرﺟﺔ‬
،‫اﻟﺤﺮارة‬
‫وﻻﺣﻆ‬
‫ﱠ‬‫أن‬
‫إﺷﺎرة‬
)
ΔH
(
‫ﺗﺸﺎﺑﮫ‬
‫إﺷﺎرة‬
)
ΔG
(
‫ﻓﻲ‬
.‫اﻟﻐﺎﻟﺐ‬
:‫ﻣﮭﻣﺔ‬ ‫ﻣﻼﺣظﺎت‬
ΔG .1
=
‫ﺳﺎﻟﺒﺔ‬
(-)
‫اﻟﺘﻔﺎﻋﻞ‬
،‫ﺗﻠﻘﺎﺋﻲ‬
ΔG
=
‫ﻣﻮﺟﺒﺔ‬
(+)
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻏﯿﺮ‬
‫ﺗﻠﻘﺎﺋﻲ‬
2
.
:‫ﻋﻤﻠﯿﺎت‬
‫)اﻻﻧﺼﮭﺎر‬
/
‫اﻟﺘﺒﺨﺮ‬
(‫)اﻟﻐﻠﯿﺎن‬
/
‫اﻟﺘﺴﺎﻣﻲ‬
(...
ΔS
=
(+)
‫ﺗﺰداد‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
ΔH
=
(+)
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻣﺎص‬
3
.
‫ﻋﻤﻠﯿﺎت‬
‫)اﻻﻧﺠﻤﺎد‬
‫)اﻟﺘﺒﻠﻮر‬
/
‫اﻟﺘﻜﺜﯿﻒ‬
(‫)اﻟﻨﺪى‬
/
‫اﻟﺘﺼﻠﺐ‬
(...
ΔS
=
(-)
‫ﺗﻘﻞ‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
ΔH
=
(-)
‫ﺑﺎﻋﺚ‬
‫ﻟﻠﺤﺮارة‬
4
.
‫ﺣﯿﻨﻤﺎ‬
:‫ﯾﻘﻮل‬
‫)ﯾﺴﺒﺐ‬
‫اﻧﺨﻔﺎض‬
‫درﺟﺔ‬
‫ﺣﺮارة‬
:(‫اﻟﻤﺤﻠﻮل‬
‫ﺑﺎﻋﺜﺔ‬ ‫واﻟﻌﻜﺲ‬ ‫ﻣﺎﺻﺔ‬ ‫اﻟﻌﻤﻠﯿﺔ‬
)
ΔH > TΔS
(
5
.
‫ذوﺑﺎن‬
‫ﺻﻠﺐ‬
‫أو‬
،‫ﺳﺎﺋﻞ‬
‫ﺗﺰداد‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
+)
=
ΔS
(
‫وﻋﻠﻰ‬
‫اﻷﻏﻠﺐ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻣﺎص‬
+)
=
ΔH
(
6
.
‫ذوﺑﺎن‬
،‫ﻏﺎز‬
‫ﺗﻘﻞ‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
-)
=
ΔS
،(
‫وھﻲ‬
:‫ﻋﻤﻠﯿﺎت‬
‫ﺑﺎﻋﺜﺔ‬
-)
=
ΔH
(
7
.
‫ﻋﻤﻠﯿﺎت‬
‫)اﻟﺘﺤﻠﻞ‬
/
‫اﻟﺘﻔﻜﻚ‬
/
:(‫اﻟﺘﺄﯾﻦ‬
‫)ﺗﺰداد‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
+)
=
ΔS
(
‫واﻟﺘﻔﺎﻋﻞ‬
‫ﻣﺎص‬
+)
=
ΔH
(
8
.
:‫ﻋﻤﻠﯿﺎت‬
‫)اﻻﺗﺤﺎد‬
/
‫اﻻﻧﺪﻣﺎج‬
:(...
‫ﺗﻘﻞ‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
-)
=
ΔH
(
9
.
‫أھم‬
:‫ﻣﻼﺣظﺔ‬
‫)إن‬
‫ﻛﺎﻧﺖ‬
‫اﻟﻌﺒﺎرات‬
‫ﻣﻨﻔﯿﺔ‬
‫ﻓﺎﻟﺘﻔﺎﻋﻞ‬
‫ﻏﯿﺮ‬
‫ﺗﻠﻘﺎﺋﻲ‬
+)
=
ΔG
،(
‫وﻧﺮﻓﻊ‬
‫اﻟﻨﻔﻲ‬
ً‫ﺎ‬‫ﻣﺆﻗﺘ‬
‫ﺛﻢ‬
‫ﻧﺤﻞ‬
‫اﻟﻤﺴﺄﻟﺔ‬
‫ﻋﻠﻰ‬
.(‫اﻟﻘﺎدﻣﺔ‬ ‫اﻟﻤﺴﺎﺋﻞ‬ ‫ﻣﻦ‬ ‫ذﻟﻚ‬ ‫ﺳﯿﺘﻮﺿﺢ‬ ‫ﻛﻤﺎ‬ ،‫ﻛﺒﺲ‬ ‫ﻋﻼﻗﺔ‬ ‫ﺿﻮء‬
‫اﻟراﺑﻊ‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
‫اﻟﺗﻔﺎﻋل‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫ﯾﺿﻣﻧﺎن‬ ‫ﻋﺎﻣﻠﯾن‬ ‫أﻛﺛر‬ ‫ھﻣﺎ‬ ‫ﻣﺎ‬
)
A
Δ𝐻°𝑟
& Δ𝐶°𝑟
)
B
∆𝐻°𝑟
& Δ𝑆°𝑟
)
C
∆𝐺°𝑟
& Δ𝑆°𝑟
(‫)ﺧﯾﺎرات‬ ‫اﻟﺳؤال‬ ‫ﻧوع‬
‫اﻟﺟواب‬
/
B
2
.
‫اﻟﺗﺻﻠب‬ / (‫)اﻟﻧدى‬ ‫اﻟﺗﻛﺛﯾف‬ / ‫)اﻟﺗﺑﻠور‬ ‫)اﻻﻧﺟﻣﺎد‬ ‫ﻋﻣﻠﯾﺎت‬
(...
ΔS
=
(+)
‫ﺗزداد‬
‫اﻟﻌﺷواﺋﯾﺔ‬
ΔH
=
(-)
‫ﺑﺎﻋث‬
‫ﻟﻠﺣرارة‬
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
F
3
.
،‫ﻏﺎز‬ ‫ذوﺑﺎن‬
‫ﺗﻘل‬
‫اﻟﻌﺷواﺋﯾﺔ‬
-)
=
ΔS
،(
‫وھﻲ‬
:‫ﻋﻣﻠﯾﺎت‬
‫ﺑﺎﻋﺛﺔ‬
-)
=
ΔH
(
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
T
(‫اﻟﺧﺎﻣس‬ ‫)اﻟدرس‬
‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫وﻓق‬ ‫ﺗﻌﺎﻟﯾل‬
‫ﻋﻠل‬
‫ﻣﺎ‬
‫ﯾﺄﺗﻲ‬
‫ﻋﻠﻰ‬
‫وﻓق‬
‫ﻋﻼﻗﺔ‬
:‫ﻛﺑس‬
‫س‬/
3
1
.
‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺟﻠﯾد‬ ‫اﻧﺻﮭﺎر‬ ‫ﻋﻣﻠﯾﺔ‬
/‫ج‬
-
‫ﺗﻠﻘﺎﺋﯿﺔ‬
ΔG
=
‫ﺳﺎﻟﺒﺔ‬
‫)اﻟﺘﻔﺎﻋﻞ‬
(‫ﺗﻠﻘﺎﺋﻲ‬
-
‫اﻧﺼﮭﺎر‬
ΔS
=
‫ﻣﻮﺟﺒﺔ‬
‫)ﺗﺰداد‬
(‫اﻟﻌﺸﻮاﺋﯿﺔ‬
-
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﻣﺎﺻﺔ‬
ΔH
=
‫ﻣﻮﺟﺒﺔ‬
ΔG = ΔH - TΔS
+ (-) + = -
ΔH < TΔS
2
.
‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫اﻷوﻟﯾﺔ‬ ‫ﻋﻧﺎﺻره‬ ‫إﻟﻰ‬ ‫اﻟﻣﺎء‬ ‫ﯾﺗﺣﻠل‬ ‫ﻻ‬
/‫ج‬
-
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﻏﯿﺮ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
ΔG
=
‫ﻣﻮﺟﺒﺔ‬
-
‫ﯾﺘﺤﻠﻞ‬
ΔS
=
‫ﻣﻮﺟﺒﺔ‬
‫)ﺗﺰداد‬
(‫اﻟﻌﺸﻮاﺋﯿﺔ‬
-
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﻣﺎﺻﺔ‬
‫ﻟﻠﺤﺮارة‬
ΔH
=
‫ﻣﻮﺟﺒﺔ‬
ΔG = ΔH - TΔS
+ (-) + = +
ΔH > TΔS
3
.
‫ﯾذوب‬
‫ﻏﺎز‬
‫ﻓﻲ‬
‫اﻟﻣﺎء‬
‫وﯾﺑﻌث‬
‫ﺣرارة‬
‫ﻋﺎﻟﯾﺔ‬
‫؟‬ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬ 𝑆𝑂2
/‫ج‬
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
ΔG
=
‫ﻣﻮﺟﺒﺔ‬
‫ذوﺑﺎن‬
‫ﻏﺎز‬
ΔS
=
‫ﺳﺎﻟﺒﺔ‬
‫)ﺗﻘﻞ‬
(‫اﻟﻌﺸﻮاﺋﯿﺔ‬
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﺑﺎﻋﺜﺔ‬
ΔH
=
‫ﺳﺎﻟﺒﺔ‬
ΔG = ΔH - TΔS
- (+) - = -
ΔH > TΔS
4
.
‫ﻻ‬
‫ﺗﺗﻔﻛك‬
‫ﻛﺎرﺑوﻧﺎت‬
‫اﻟﻛﺎﻟﺳﯾوم‬
‫؟‬ً‫ﺎ‬‫اﻋﺗﯾﺎدﯾ‬
/‫ج‬
‫اﻟﻌﻤﻠﯿﺔ‬
‫ﻏﯿﺮ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
ΔG
=
‫ﻣﻮﺟﺒﺔ‬
‫ﺗﺰداد‬
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
ΔS
=
‫ﻣﻮﺟﺒﺔ‬
ΔG = ΔH - TΔS
+ (-) + = +
ΔH > TΔS
:‫ﻣﮭﻤﺔ‬ ‫ﻣﻼﺣﻈﺎت‬
1
‫ﻋﻨﺪﻣﺎ‬-
‫ﺗﻜﻮن‬
‫اﺷﺎرة‬
)
(
‫ﻣﺘﺸﺎﺑﮭﺔ‬ ∆𝐻, ∆𝑆
a) ∆𝐻 =−
∆𝑆 =−
∆𝐺 = ∆𝐻 − 𝑇∆𝑆
−
( ) − −
( )
−
( ) (+)
‫ھﻨﺎ‬
‫ﯾﻜﻮن‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﺗﻠﻘﺎﺋﻲ‬
‫ﻋﻨﺪﻣﺎ‬
‫ﺗﻜﻮن‬
(‫)ﺗﺒﺮﯾﺪ‬ ∆𝐻 > 𝑇∆𝑆
b) ∆𝐻 =+
∆𝑆 =+
∆𝐺 = ∆𝐻 − 𝑇∆𝑆
+
( ) − +
( )
+
( ) (−)
‫ھﻨﺎ‬
‫ﯾﻜﻮن‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﺗﻠﻘﺎﺋﻲ‬
‫ﻋﻨﺪﻣﺎ‬
‫ﺗﻜﻮن‬
(‫)ﺗﺴﺨﯿﻦ‬ 𝑇∆𝑆 > ∆𝐻
‫اﻟﺧﺎﻣس‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
‫؟‬ ‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺟﻠﯾد‬ ‫اﻧﺻﮭﺎر‬ ‫ﻋﻣﻠﯾﺔ‬
)
A
‫ﺗﻠﻘﺎﺋﯾﺔ‬
ΔG
=
‫ﺳﺎﻟﺑﺔ‬
‫)اﻟﺗﻔﺎﻋل‬
(‫ﺗﻠﻘﺎﺋﻲ‬
-
‫اﻧﺻﮭﺎر‬
ΔS
=
‫ﻣوﺟﺑﺔ‬
‫)ﺗزداد‬
(‫اﻟﻌﺷواﺋﯾﺔ‬
-
‫اﻟﻌﻣﻠﯾﺔ‬
‫ﻣﺎﺻﺔ‬
ΔH
=
‫ﺳﺎﻟﺑﺔ‬
ΔG = ΔH - TΔS
+ (-) + = -
ΔH > TΔS
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
F
2
.
‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫اﻷوﻟﯾﺔ‬ ‫ﻋﻧﺎﺻره‬ ‫إﻟﻰ‬ ‫اﻟﻣﺎء‬ ‫ﯾﺗﺣﻠل‬ ‫ﻻ‬
:‫ﺑﺳﺑب‬ ‫وذﻟك‬
)
A
‫اﻟﻌﻣﻠﯾﺔ‬
‫ﺗﻠﻘﺎﺋﯾﺔ‬
ΔG
=
‫ﻣوﺟﺑﺔ‬
-
‫ﯾﺗﺣﻠل‬
ΔS
=
‫ﻣوﺟﺑﺔ‬
‫)ﺗزداد‬
(‫اﻟﻌﺷواﺋﯾﺔ‬
)
B
‫اﻟﻌﻣﻠﯾﺔ‬
‫ﻏﯾر‬
‫ﺗﻠﻘﺎﺋﯾﺔ‬
ΔG
=
‫ﻣوﺟﺑﺔ‬
-
‫ﯾﺗﺣﻠل‬
ΔS
=
‫ﻣوﺟﺑﺔ‬
‫)ﺗزداد‬
(‫اﻟﻌﺷواﺋﯾﺔ‬
-
‫اﻟﻌﻣﻠﯾﺔ‬
‫ﻣﺎﺻﺔ‬
‫ﻟﻠﺣرارة‬
ΔH
=
‫ﻣوﺟﺑﺔ‬
( ‫اﻟﺳﺎدس‬ ‫)اﻟدرس‬
‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫ﺣﺳﺎﺑﺎت‬
:‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫ﺣﺳﺎﺑﺎت‬
‫ﯾﻤﻜﻦ‬
‫اﺳﺘﺨﺪام‬
‫ﻋﻼﻗﺔ‬
‫ﻛﺒﺲ‬
‫ﻟﺤﺴﺎب‬
‫ﻗﯿﻤﺔ‬
‫اﻟﻄﺎﻗﺔ‬
‫اﻟﺤﺮة‬
Δ
‫اﻟﻘﯿﺎﺳﯿﺔ‬
‫وﺑﺎﻟﺘﺎﻟﻲ‬
‫ﻣﻌﺮﻓﺔ‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
‫أو‬
‫ﻋﺪم‬
‫ﺗﻠﻘﺎﺋﯿﺔ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫وذﻟﻚ‬ 𝐺𝑟
°
‫إذا‬
‫ﺗﻢ‬
‫ﻗﯿﺎس‬
‫ﻗﯿﻢ‬
Δ
‫و‬
،
‫ﻋﻨﺪ‬
‫اﻟﻈﺮوف‬
‫اﻟﻘﯿﺎﺳﯿﺔ‬
)
1
atm/25
(
،
‫وذﻟﻚ‬
‫ﻣﻦ‬
‫ﺧﻼل‬
‫اﻟﻌﻼﻗﺔ‬
:‫اﻟﺘﺎﻟﯿﺔ‬ 𝐻𝑟
°
∆𝑆𝑟
°
℃
∆𝐺𝑟
°
= ∆𝐻𝑟
°
− 𝑇∆𝑆𝑟
°
‫ﻣﻼﺣظﺔ‬
1
/
‫ﯾﺠﺐ‬
‫اﻟﺘﻤﯿﯿﺰ‬
‫ﺑﯿﻦ‬
Δ
‫و‬
‫وﺑﯿﻦ‬
Δ
‫و‬
Δ
. 𝐺𝑟
°
∆𝐺𝑓
°
𝐻𝑟
°
𝐻𝑓
°
‫ﻣﻼﺣظﺔ‬
2
/
‫ﻗﯿﻢ‬
‫اﻻﻧﺜﺎﻟﺒﻲ‬
‫واﻟﻄﺎﻗﺔ‬
‫اﻟﺤﺮة‬
‫ﻟﻠﻌﻨﺎﺻﺮ‬
‫اﻟﺤﺮة‬
‫ﺑﺄﺛﺒﺖ‬
‫ﺻﻮرة‬
‫ﺗﺴﺎوي‬
‫ﺻﻔﺮ‬
‫ﻣﻼﺣظﺔ‬
3
/
‫ﯾﺠﺐ‬
‫ﺗﻮﺣﯿﺪ‬
‫وﺣﺪﺗﻲ‬
‫و‬
Δ
‫ﻗﺒﻞ‬
‫ﺗﻄﺒﯿﻖ‬
‫ﻋﻼﻗﺔ‬
.‫ﻛﺒﺲ‬ ∆𝑆𝑟
°
𝐺𝑟
°
‫ﻣﻼﺣظﺔ‬
4
/
‫اﻟﻌﺸﻮاﺋﯿﺔ‬
(‫)اﻻﻧﺘﺮوﺑﻲ‬
‫ﻟﻠﺠﺰﯾﺌﺎت‬
‫ﺗﻌﺘﻤﺪ‬
‫ﻋﻠﻰ‬
‫اﻟﻄﺎﻗﺔ‬
،‫اﻟﺤﺮﻛﯿﺔ‬
‫وھﻲ‬
‫ﺣﺮﻛﺎت‬
‫ﺻﻐﯿﺮة‬
‫ﺑﺎﻟﻨﺴﺒﺔ‬
‫ﻟﻘﯿﻢ‬
‫اﻻﻧﺜﺎﻟﺒﻲ‬
‫واﻟﻄﺎﻗﺔ‬
‫اﻟﺤﺮة‬
‫ﻟﺬﻟﻚ‬
‫ﺗﻜﻮن‬
‫وﺣﺪة‬
ΔS
‫ﺻﻐﯿﺮة‬
‫ﺑﺎﻟﺠﻮل‬
)
J
(
‫ووﺣﺪات‬
ΔH
‫و‬
ΔG
‫ﻛﺒﯿﺮة‬
‫ﺑﺎﻟـ‬
)
KJ
.(
‫س‬
4
/
‫ﺟد‬
‫ﻗﯾﻣﺔ‬
)
(
‫ﻟﻠﺗﻔﺎﻋل‬
:‫اﻟﺗﺎﻟﻲ‬ ∆𝐺°𝑟
2𝐶𝑂(𝑔)
+ 𝑂2
(𝑔)
→ 2𝐶𝑂2
(𝑔)
‫اﻟﻣﻌﻠوﻣﺎت‬ ‫أﻋطﯾت‬ ‫إذا‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻟظروف‬ ‫ﺗﺣت‬ ‫ﯾﺟري‬ ‫اﻟذي‬
:‫اﻵﺗﯾﺔ‬
Δ
=
-)
110.5
(
KJ/mol
, 𝐻𝑓𝐶𝑂
°
Δ
=
-)
393.5
(
KJ/mol 𝐻𝑓𝐶𝑂2
°
=
198
J/K mol
, 𝑆𝐶𝑂
°
=
214
J/K mol
, 𝑆𝐶𝑂2
°
=
205
J/K mol 𝑆𝑂2
°
/‫اﻟﺣل‬
1
-
Δ
𝐻𝑟
°
= 2∆𝐻𝑓𝐶𝑂2
°
⎡
⎢
⎣
⎤
⎥
⎦
− 2∆𝐻𝑓𝐶𝑂
°
( )+ ∆𝐻𝑓𝑂2
°
( )
⎡
⎢
⎣
⎤
⎥
⎦
Δ
𝐻𝑟
°
= 2 × − 393. 5
( )
[ ] − 2 × − 110. 5
( ) + 0
[ ]
Δ
𝐻𝑟
°
= − 787
( ) + 221
( )
∆𝐻𝑟
°
= − 566 𝐾𝐽/𝑚𝑜𝑙
2. ∆𝑆𝑟
°
= 2𝑆𝐶𝑂2
°
⎡
⎢
⎣
⎤
⎥
⎦
− 2𝑆𝐶𝑂
°
+ 𝑆𝑂2
°
⎡
⎢
⎣
⎤
⎥
⎦
∆𝑆𝑟
°
= [2 × 214] − [2 × 198) + 205]
∆𝑆𝑟
°
= − 173 𝐽/𝐾 𝑚𝑜𝑙
= -0.173 KJ/K mol ‫ﻧﻮﺣﺪ‬
‫اﻟﻮﺣﺪات‬
∆𝑆𝑟
°
=
−173
1000
3. Δ
∴ 𝐺𝑟
°
= ∆𝐻𝑟
°
− 𝑇 ∆𝑆𝑟
°
,
𝑇𝑘
= 𝑡℃ + 273
𝑇𝑘
= 25 + 273 = 298𝐾
= -566 - (298) (-0.173)
Δ
∴ 𝐺𝑟
°
= − 514. 446
𝐾𝐽
𝑚𝑜𝑙
(‫ﺗﻠﻘﺎﺋﻲ‬ ‫)اﻟﺘﻔﺎﻋﻞ‬
‫س‬
5
/
‫ﻟﻠﺗﻔﺎﻋل‬
‫اﻟﺗﺎﻟﻲ‬
2𝐻2
𝑔
( )
+ 𝑂2
(𝑔)
→ 2𝐻2
𝑂(𝑔)
(J/K.mol) ‫ﻟﻠﺗﻔﺎﻋل‬
‫ﺑوﺣدة‬ ‫اﺣﺳب‬
‫ﻗﯾﻣﺔ‬
∆𝑆𝑟
°
:‫ﻋﻠﻣت‬ ‫إذا‬
Δ𝐻𝑓𝐻2
𝑂
°
= − 242
( )𝐾𝐽/𝑚𝑜𝑙)
Δ𝐺𝑓𝐻2
𝑂
°
= − 228
( )𝐾𝐽/𝑚𝑜𝑙)
/‫اﻟﺣل‬
Δ
𝐻𝑟
°
= ∑ 𝑛∆𝐻𝑓(𝑃)
°
− ∑ 𝑛 ∆𝐻𝑓(𝑅)
°
=
]
2Δ
[𝐻𝑓𝐻2
𝑂
°
− [2∆𝐻𝑓𝐻2
°
+ ∆𝐻𝑓𝑂2
°
]
Δ
𝐻𝑟
°
= [2(− 242)] − [0]⟹∆𝐻𝑟
°
= − 484 𝐾𝐽/𝑚𝑜𝑙
Δ
𝐺𝑟
°
= ∑ 𝑛 ∆𝐺𝑓(𝑃)
°
∑ 𝑛 ∆𝐺𝑓(𝑅)
°
=
]
2Δ
[
−
]
0
+
0
[ 𝐺𝑓𝐻2
𝑂
°
T = 25 + 273
T = 298 K
Δ
𝐺𝑟
°
= [2(− 228)]⟹∆𝐺𝑟
°
= − 456 𝐾𝐽/𝑚𝑜𝑙
Δ
𝐺𝑟
°
= ∆𝐻𝑟
°
− 𝑇∆𝑆𝑟
°
-
456
=
-
484
-
)
298
(
∆𝑆𝑟
°
⟹ ∆𝑆𝑟
°
=
−28
298
= − 0. 094 𝐾𝐽/𝐾 𝑚𝑜𝑙
∴ ∆𝑆𝑟
°
= − 0. 094 × 1000⟹ ∆𝑆𝑟
°
= − 94 𝐽/𝐾 𝑚𝑜𝑙
‫اﻟﺳﺎدس‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
Δ𝐺𝑟
°
= Δ𝐻𝑟
°
− 𝑇∆𝑆𝑟
°
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
T
2
.
)
A
‫ﯾﺟب‬
‫اﻟﺗﻣﯾﯾز‬
‫ﺑﯾن‬
Δ
‫و‬
‫وﺑﯾن‬
Δ
‫و‬
Δ
. 𝐺𝑟
°
∆𝐺°𝑓
𝐻𝑟
°
𝐻𝑓
°
)
B
‫ﻗﯾم‬
‫اﻻﻧﺛﺎﻟﺑﻲ‬
‫واﻟطﺎﻗﺔ‬
‫اﻟﺣرة‬
‫ﻟﻠﻌﻧﺎﺻر‬
‫اﻟﺣرة‬
‫ﺑﺄﺛﺑت‬
‫ﺻورة‬
‫ﺗﺳﺎوي‬
1
)
C
‫ﻗﯾم‬
‫اﻻﻧﺛﺎﻟﺑﻲ‬
‫واﻟطﺎﻗﺔ‬
‫اﻟﺣرة‬
‫ﻟﻠﻌﻧﺎﺻر‬
‫اﻟﺣرة‬
‫ﺑﺄﺛﺑت‬
‫ﺻورة‬
‫ﺗﺳﺎوي‬
‫ﺻﻔر‬
(‫)ﺧﯾﺎرات‬ ‫اﻟﺳؤال‬ ‫ﻧوع‬
‫اﻟﺟواب‬
/
A& C
3
.
‫اﻟطﺎﻗﺔ‬ ‫ﻋﻠﻰ‬ ‫ﺗﻌﺗﻣد‬ ‫ﻻ‬ ‫ﻟﻠﺟزﯾﺋﺎت‬ (‫)اﻻﻧﺗروﺑﻲ‬ ‫اﻟﻌﺷواﺋﯾﺔ‬
‫ﺻﻐﯾرة‬ ‫ﺣرﻛﺎت‬ ‫وھﻲ‬ ،‫اﻟﺣرﻛﯾﺔ‬
‫اﻟﺣرة‬ ‫واﻟطﺎﻗﺔ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﻟﻘﯾم‬ ‫ﺑﺎﻟﻧﺳﺑﺔ‬
‫ﻟذﻟك‬
‫ﺗﻛون‬
‫وﺣدة‬
ΔS
‫ﺻﻐﯾرة‬
‫ﺑﺎﻟﺟول‬
)
J
(
‫ووﺣدات‬
ΔH
‫و‬
ΔG
‫ﻛﺑﯾرة‬
‫ﺑﺎﻟـ‬
)
KJ
.(
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
F
( ‫اﻟﺳﺎﺑﻊ‬ ‫)اﻟدرس‬
‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬
‫س‬
6
/
‫ﺟﺪ‬
‫درﺟﺔ‬
‫اﻟﺤﺮارة‬
‫اﻟﺘﻲ‬
‫ﺗﺼﺒﺢ‬
‫ﻋﻨﺪھﺎ‬
‫اﻟﺘﻔﺎﻋﻼت‬
‫اﻟﺘﺎﻟﯿﺔ‬
،‫ﺗﻠﻘﺎﺋﯿﺔ‬
‫إذا‬
:‫ﻋﻠﻤﺖ‬
‫ﻓرع‬
)
A
/(
∆𝐻𝑟
= (+ 126) 𝐾𝐽/𝑚𝑜𝑙
∆𝑆𝑟
= (+ 48) 𝐽/𝐾 𝑚𝑜𝑙
/‫اﻟﺣل‬
ΔG ‫ﻧﻔﺘﺮض‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻓﻲ‬
‫ﺣﺎﻟﺔ‬
،‫اﺗﺰان‬
،
‫ﺻﻔﺮ‬ =
∴
‫وﻧﻮﺣﺪ‬
‫اﻟﻮﺣﺪات‬
∆𝐻
∆𝑆
= 𝑇⟹ 0 = ∆𝐻 − ∆𝑆
∆𝑆𝑟
=
48
1000
⟹ ∆𝑆𝑟
= + 0. 048 𝐾𝐽/𝐾 𝑚𝑜𝑙
∴ 𝑇 =
126
0.048
⟹ 𝑇 = 2625 𝐾
/‫ﻣﻼﺣظﺔ‬
‫إذا‬
‫ﻛﺎﻧﺖ‬
‫إﺷﺎرة‬
ΔS
‫و‬
ΔH
=
‫ﻣﻮﺟﺒﺔ‬
‫ﻓﯿﺠﺐ‬
‫ﺗﺴﺨﯿﻦ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻷﻛﺜﺮ‬
‫ﻣﻦ‬
‫درﺟﺔ‬
‫اﻟﺤﺮارة‬
‫اﻟﻤﺤﺴﻮﺑﺔ‬
‫ﻋﻨﺪ‬
‫اﻻﺗﺰان‬
.
‫وﻋﻠﯿﮫ‬
‫ﯾﺠﺐ‬
‫ﺗﺴﺨﯿﻦ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻷﻛﺜﺮ‬
‫ﻣﻦ‬
)
2625
K
(
‫ﻟﻜﻲ‬
‫ﯾﺼﺒﺢ‬
‫اﻟﺘﻔﺎﻋﻞ‬
.‫ﺗﻠﻘﺎﺋﻲ‬
(B) ‫ﻓرع‬/
∆𝑆𝑟
= (− 105) 𝐽/𝐾 𝑚𝑜𝑙, ∆𝐻𝑟
= (− 12) 𝐾𝐽/𝑚𝑜𝑙
‫ﻧﻔﺘﺮض‬
ΔG
=
‫ﺻﻔﺮ‬
‫)ﺣﺎﻟﺔ‬
(‫اﻻﺗﺰان‬
∴ 𝑇 =
∆𝐻
∆𝑆
, ∆𝑆 =
−105
1000
⟹ ∆𝑆 = − 0. 105 𝐾𝐽/𝐾 𝑚𝑜𝑙
𝑇 =
−12
−0.105
⟹ 𝑇 = 114. 3 𝐾
‫وﻋﻠﯿﮫ‬
‫ﯾﺠﺐ‬
‫ﺗﺒﺮﯾﺪ‬
‫إﻧﺎء‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻷﻗﻞ‬
‫ﻣﻦ‬
)
114.3
K
(
‫ﻟﯿﺼﺒﺢ‬
‫اﻟﺘﻔﺎﻋﻞ‬
.‫ﺗﻠﻘﺎﺋﻲ‬
‫داﺋﻤﺎ‬
‫ﻓﻲ‬
‫اﻟﺴﺆال‬
‫ﻣﺘﺸﺎﺑﮭﺔ‬ ΔS ‫و‬ ΔH ‫ﺳﺘﻌﻄﻰ‬
‫أﺷﺎرات‬
‫ﻗﯿﻢ‬
‫ﻣﻼﺣظﺔ‬/
= ‫ﺳﺎﻟﺒﺔ‬
‫)ﻧﺒﺮداﻟﺘﻔﺎﻋﻞ‬ ) ΔS ‫و‬ ΔH ‫اذا‬
‫ﻛﺎﻧﺖ‬
‫س‬
7
:
‫ﺗﺘﻔﻜﻚ‬
‫ﻛﺎرﺑﻮﻧﺎت‬
‫اﻟﻜﺎﻟﺴﯿﻮم‬
‫ﺣﺴﺐ‬
‫اﻟﻤﻌﺎدﻟﺔ‬
‫اﻵﺗﯿﺔ‬ :
𝐶𝑎𝐶𝑂3
(𝑠)
∆→ 𝐶𝑎𝑂(𝑠)
+ 𝐶𝑂2
(𝑔)
(160 J/K mol) =Δ𝑆°𝑟
‫ﻓﺈذا‬
‫ﻋﻠﻤﺖ‬
Δ
‫ﻟﻜﻞ‬
‫ﻣﻦ‬
‫و‬
CaO
‫و‬
‫ھﻲ‬
‫ﻋﻠﻰ‬
:‫اﻟﺘﻮاﻟﻲ‬ 𝐻𝑓
°
𝐶𝑂2
𝐶𝑎𝐶𝑂3
-)
1207
/
-
635
/
-
393.5
(
‫ﺑﻮﺣﺪات‬
KJ/mol
،
:‫ﺟﺪ‬
‫ﻟﻠﺘﻔﺎﻋﻞ‬
‫ﺛﻢ‬
‫أرﺳﻢ‬
‫ﻣﺨﻄﻂ‬
‫اﻟﻄﺎﻗﺔ‬ Δ 1)
𝐻𝑟
°
‫ﻟﻠﺘﻔﺎﻋﻞ‬Δ 2)
𝐺𝑟
°
3) ‫درﺟﺔ‬
‫اﻟﺤﺮارة‬
‫اﻟﺘﻲ‬
‫ﯾﺼﺒﺢ‬
‫ﻋﻨﺪھﺎ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﺗﻠﻘﺎﺋﯿﺎ‬
/‫اﻟﺣل‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻣﺎص‬
1
(
∆𝐻𝑟
°
= ∑ 𝑛∆ 𝐻𝑓(𝑃)
°
− ∑ 𝑛 ∆𝐻𝑓 𝑅
( )
°
∆𝐻𝑟
°
= [(− 635) + (− 393. 5)] − [− 1207]
∆𝐻𝑟
°
= (− 1028) + (1207)
∆𝐻𝑟
°
= 178. 5 𝐾𝐽/𝑚𝑜𝑙
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻏﯿﺮ‬
‫ﺗﻠﻘﺎﺋﻲ‬
2
(
T = 25 + 273 = 298 K
∆𝑆𝑟
°
=
160
1000
= 0. 16 𝐾𝐽/𝐾 𝑚𝑜𝑙
∴ ∆𝐺𝑟
°
= ∆𝐻𝑟
°
− 𝑇∆𝑆𝑟
°
∆𝐺𝑟
°
= 178. 5 − (298) (0. 16)
∆𝐺𝑟
°
= 130. 82 𝐾𝐽/𝑚𝑜𝑙
3) (0 = Δ ‫ﻧﻔﺘﺮض‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫ﻣﺘﺰن‬
𝐺𝑟
°
)
0 = ∆𝐻𝑟
°
− 𝑇∆𝑆⟹𝑇 =
∆𝐻𝑟
°
∆𝑆𝑟
° ⟹ 𝑇 =
178.5
0.16
= 115. 6 𝐾
‫ﻣﻮﺟﺒﺔ‬Δ ‫و‬ ‫ﺑﻤﺎ‬
‫اﻧﮫ‬
‫ﻗﯿﻤﺘﻲ‬
𝐻𝑟
°
∆𝑆𝑟
°
‫ﻟﻜﻲ‬
‫ﯾﺼﺒﺢ‬
‫اﻟﺘﻔﺎﻋﻞ‬
.ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯿ‬
1115.6 K ً‫ا‬‫إذ‬
‫ﯾﺠﺐ‬
‫ﺗﺴﺨﯿﻦ‬
‫اﻟﺘﻔﺎﻋﻞ‬
‫إﻟﻰ‬
‫أﻛﺜﺮ‬
‫ﻣﻦ‬
‫اﻟﺳﺎﺑﻊ‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
1
.
‫إذا‬
‫ﻛﺎﻧت‬
‫إﺷﺎرة‬
ΔS
‫و‬
ΔH
=
‫ﺳﺎﻟﺑﺔ‬
‫ﻓﯾﺟب‬
‫ﺗﺳﺧﯾن‬
‫اﻟﺗﻔﺎﻋل‬
‫ﻷﻛﺛر‬
‫ﻣن‬
‫درﺟﺔ‬
‫اﻟﺣرارة‬
.‫اﻻﺗزان‬ ‫ﻋﻧد‬ ‫اﻟﻣﺣﺳوﺑﺔ‬
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
F
2
.
‫اذا‬
‫ﻛﺎﻧت‬
S Δ
‫و‬
ΔH
=
‫ﺳﺎﻟﺑﺔ‬
(‫)ﻧﺑرداﻟﺗﻔﺎﻋل‬
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
F
3
.
‫ﯾﺟب‬
‫ﺗﺳﺧﯾن‬
‫اﻟﺗﻔﺎﻋل‬
‫ﻷﻛﺛر‬
‫ﻣن‬
)
2625
K
(
‫ﻟﻛﻲ‬
‫ﯾﺻﺑﺢ‬
‫اﻟﺗﻔﺎﻋل‬
.‫ﺗﻠﻘﺎﺋﻲ‬
‫ﻧوع‬
‫اﻟﺳؤال‬
)
T, F
(
‫اﻟﺟواب‬
/
T

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  • 1. ‫اﻟﻔﺻل‬ ‫اﻻول‬ ‫اﻟﺛرﻣوداﯾﻧﻣك‬ ( ‫اﻟدرس‬ ‫اﻷول‬ ) ‫اﻟﺛرﻣوداﯾﻧﻣك‬ ‫طرﯾﻘﺔ‬ ‫ﻗﺎﻧون‬ ‫ھﯾس‬ : /‫ﺳؤال‬ ‫ﻟﻣﺎذا‬ ‫ﯾﺗم‬ ‫اﻟﻠﺟوء‬ ‫إﻟﻰ‬ ‫طرﯾﻘﺔ‬ ‫ھﯾس‬ ‫ﻟﺣﺳﺎب‬ Δ ‫𝐻؟‬𝑟 ° ‫ﺟواب‬ / ‫ﱠ‬‫ﻷن‬ ‫ﺑﻌض‬ ‫اﻟﻣرﻛﺑﺎت‬ ‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬ ‫ﻻ‬ ‫ﯾﻣﻛن‬ ‫ﺗﺻﻧﯾﻌﮭﺎ‬ ً‫ة‬‫ﻣﺑﺎﺷر‬ ‫ﻣن‬ ‫ﻋﻧﺎﺻرھﺎ‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﺑﺄﺛﺑت‬ ‫ﺻورة‬ (‫)ﻋﻠل‬ ‫ﺑﺳﺑب‬ : ‫ﱠ‬‫أن‬ 1 ( ‫ﺑﻌض‬ ‫اﻟﺗﻔﺎﻋﻼت‬ ‫ﺗﺳﯾر‬ ‫ﺑﺑطء‬ .‫ﺷدﯾد‬ 2 ( ‫ن‬ ّ‫ﺗﻛو‬ ‫ﻣرﻛﺑﺎت‬ ‫ﺟﺎﻧﺑﯾﺔ‬ ‫ﻏﯾر‬ ‫ﻣرﻏوب‬ .‫ﻓﯾﮭﺎ‬ ‫ھﯾس؟‬ ‫ﻗﺎﻧون‬ ‫ﻧص‬ ‫ھو‬ ‫ﻣﺎ‬ :‫ﯾﻧص‬ ‫)ﻋﻧد‬ ‫ﺗﺣوﯾل‬ ‫اﻟﻣﺗﻔﺎﻋﻼت‬ ‫إﻟﻰ‬ ‫ﻧواﺗﺞ‬ ‫ﱠ‬‫ﻓﺈن‬ ‫اﻟﺗﻐﯾر‬ ‫ﻓﻲ‬ ‫اﻧﺛﺎﻟﺑﻲ‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ھو‬ ‫ﻧﻔﺳﮫ‬ ‫ﺳواء‬ ‫ﺗم‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻓﻲ‬ ‫ﺧطوة‬ ‫واﺣدة‬ .(‫اﻟﺧطوات‬ ‫ﻣن‬ ‫ﺳﻠﺳﻠﺔ‬ ‫ﻋﺑر‬ ‫أو‬ / ‫ﻣﺛﺎل‬ 𝐶‫ﻛﺮاﻓﯿﺖ‬ + 𝑂2 (𝑔) ⟶𝐶𝑂2 𝑔 ( ) ∆𝐻𝑟 =− 393. 5 𝐾𝐽/𝑚𝑜𝑙 ‫وﻋﻧد‬ ‫ﺗﻛوﯾن‬ ‫ﺑﺄﻛﺛر‬ ‫ﻣن‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﻓﺄن‬ ‫ھو‬ ‫ﻧﻔﺳﮫ‬ 𝐶𝑂2 ∆𝐻𝑟 𝐶‫ﻛﺮاﻓﯿﺖ‬ + 1 2 𝑂2 (𝑔) ⟶𝐶𝑂 𝑔 ( ) ∆𝐻𝑟 =− 110. 5 𝐾𝐽/𝑚𝑜𝑙 𝐶𝑂 𝑔 ( ) + 1 2 𝑂2 (𝑔) ⟶𝐶𝑂2 𝑔 ( ) ∆𝐻𝑟 =− 283 𝐾𝐽/𝑚𝑜𝑙 𝐶‫ﻛﺮاﻓﯿﺖ‬ + 𝑂2 (𝑔) ⟶𝐶𝑂2 𝑔 ( ) ∆𝐻𝑟 =− 393. 5 𝐾𝐽/𝑚𝑜𝑙
  • 2. ‫ھﯾس‬ ‫ﻣﺳﺎﺋل‬ ‫ﺣل‬ ‫ﺣول‬ ‫ﻣﮭﻣﺔ‬ ‫ﻣﻼﺣظﺎت‬ : 1 ( ‫ﻋﻧد‬ ‫ﻗﻠب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﻧﻘﻠب‬ ‫إﺷﺎرة‬ ‫ﻗﯾﻣﺔ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ . 2 ( ‫ﻋﻧد‬ ‫ﺿرب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫أو‬ ‫ﻗﺳﻣﺗﮭﺎ‬ ‫ﻋﻠﻰ‬ ‫ﻣﻌﺎﻣل‬ ‫ﻋددي‬ ‫ﻓﺗﺿرب‬ ‫أو‬ ‫ﺗﻘﺳم‬ ‫ﻗﯾﻣﺔ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﺑﻧﻔس‬ .‫اﻟﻌدد‬ 3 ( ‫ھﻧﺎك‬ ‫ﻧوﻋﺎن‬ ‫ﻣن‬ :‫اﻟﻣﻌﺎدﻻت‬ :‫اﻷول‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫اﻟطﻠب‬ (‫)اﻟﮭدف‬ ‫وﺗﺳﻣﻰ‬ ‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬ ،‫اﻟرﺋﯾﺳﯾﺔ‬ :‫واﻟﺛﺎﻧﻲ‬ ‫اﻟﻣﻌﺎدﻻت‬ .‫اﻟﻔرﻋﯾﺔ‬ 4 ( ‫ﻧﻣر‬ ‫ﻋﻠﻰ‬ ‫ﻣواد‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟرﺋﯾﺳﯾﺔ‬ ً‫ء‬‫اﺑﺗدا‬ ‫ﻣن‬ ‫أول‬ ،‫ﻣﺎدة‬ ‫وﻟﯾس‬ ً‫ﺎ‬‫ﺷرط‬ ‫أن‬ ‫ﻧﻣر‬ ‫ﻋﻠﻰ‬ ‫ﺟﻣﯾﻊ‬ ‫ﻣواد‬ ‫ھذه‬ .‫اﻟﻣﻌﺎدﻟﺔ‬ 5 ( ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟﻔرﻋﯾﺔ‬ ‫اﻟﺗﻲ‬ ‫ﺗم‬ ‫اﻟﺗﻌﺎﻣل‬ ‫ﻣﻌﮭﺎ‬ ‫ﻻ‬ ‫ﯾﺗم‬ ‫اﻟرﺟوع‬ ‫إﻟﯾﮭﺎ‬ .ً‫ﺛﺎﻧﯾﺔ‬ 6 ( ‫اﻟﻣﻼﺣظﺔ‬ ‫اﻷوﻟﻰ‬ :‫اﻟذھﺑﯾﺔ‬ ‫إذا‬ ‫ﺗﻛررت‬ ‫ﻣﺎدة‬ ‫ﻓﻲ‬ ‫أﻛﺛر‬ ‫ﻣن‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﻓرﻋﯾﺔ‬ ‫ﻓﯾﺗم‬ ‫ﺗﺟﺎوزھﺎ‬ ‫ﻟﻠﻣﺎدة‬ ‫اﻟﺗﻲ‬ ‫ﺗﻠﯾﮭﺎ‬ ‫ﻓﻲ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ .‫اﻟرﺋﯾﺳﯾﺔ‬ 7 ( ‫اﻟﻣﻼﺣظﺔ‬ :‫اﻟذھﺑﯾﺔ‬ ‫إذا‬ ‫ﻛﺎﻧت‬ ‫اﻟﻣﺎدة‬ ‫اﻟﻣﺗﻛررة‬ ‫ھﻲ‬ ‫آﺧر‬ ‫ﻣﺎدة‬ ‫ﻓﻲ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟرﺋﯾﺳﯾﺔ‬ ‫ﻓﺳﻧﺿطر‬ ‫ﻟﻠﺗﻌﺎﻣل‬ ‫ﻣﻌﮭﺎ‬ ‫ﺑﺷرط‬ .‫اﻟﺗﻐﯾﯾر‬ ‫ﺑﻌد‬ ‫اﻟﻔرﻋﯾﺔ‬ ‫اﻟﻣﻌﺎدﻻت‬ ‫ﻓﻲ‬ ‫ﻣوﻻﺗﮭﺎ‬ ‫ﻋدد‬ ‫ﺣﺳﺎب‬ ‫ﻣﺛﺎل‬ 1 / ‫اﺣﺳب‬ ‫اﻧﺛﺎﻟﺑﻲ‬ ‫اﻟﺗﻛوﯾن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﻣرﻛب‬ ‫ﻣن‬ ‫ﻋﻧﺎﺻره‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﺑﺄﺛﺑت‬ :‫ﺻورھﺎ‬ 𝐶𝑆2 (𝐿) Δ = ? 𝐶‫ﻛﺮاﻓﯿﺖ‬ + 2𝑆‫ﻣﻌﯿﻨﻲ‬ → 𝐶𝑆2 (𝐿) 𝐻𝑓 ° :‫اﻵﺗﯾﺔ‬ ‫اﻟﺣرارﯾﺔ‬ ‫اﻟﻣﻌﺎدﻻت‬ ‫أﻋطﯾت‬ ‫إذا‬ = - 394 KJ/mol 1 ( )𝐶‫ﻛﺮاﻓﯿﺖ‬ + 𝑂2 𝑔 ( ) →𝐶𝑂2 (𝑔) ∆𝐻𝑟 ° = - 296 KJ/mol (2) 𝑆‫ﻣﻌﯿﻨﻲ‬ + 𝑂2 𝑔 ( ) →𝑆𝑂2 (𝑔) ∆𝐻𝑟 °
  • 3. = - 1072 KJ/mol 3 ( )𝐶𝑆2 (𝐿) + 3𝑂2 (𝑔) → 𝐶𝑂2 (𝑔) + 2𝑆𝑂2 (𝑔) ∆𝐻𝑟 ° /‫اﻟﺣل‬ ‫ﺗﺑﻘﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 1 ( ‫ﻛﻣﺎ‬ ،‫ھﻲ‬ ‫وﻧﺿرب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 2 ( × 2 ، ‫وﺗﻘﻠب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 3 ( : = - 394 (1) 𝐶‫ﻛﺮاﻓﯿﺖ‬ + 𝑂2 → 𝐶𝑂2 ∆𝐻𝑟 ° KJ/mol = - 592 (2)2𝑆 + 2𝑂2 → 2𝑆𝑂2 ∆𝐻𝑟 ° KJ/mol = + 1072 KJ/mol 3 ( )𝐶𝑂2 (𝑔) + 2𝑆𝑂2 (𝑔) → 𝐶𝑆2 (𝐿) + 3𝑂2 (𝑔) ∆𝐻𝑟 ° Δ = = 86 KJ/mol 𝐶 ‫ﻛﺮاﻓﯿﺖ‬ + 𝑆‫ﻣﻌﯿﻨﻲ‬ → 𝐶𝑆2 (𝐿) 𝐻𝑓 ° ∆𝐻𝑟 ° ‫اﻻول‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬ 1 . ‫ﯾﺗم‬ ‫اﻟﻠﺟوء‬ ‫إﻟﻰ‬ ‫طرﯾﻘﺔ‬ ‫ھﯾس‬ ‫ﻟﺣﺳﺎب‬ Δ ‫ﱠ‬‫ﻷن‬ ‫ﺑﻌض‬ ‫اﻟﻣرﻛﺑﺎت‬ ‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬ ‫ﯾﻣﻛن‬ ‫ﺗﺻﻧﯾﻌﮭﺎ‬ 𝐻𝑟 ° ‫ﺻورة‬ ‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﻋﻧﺎﺻرھﺎ‬ ‫ﻣن‬ ً‫ة‬‫ﻣﺑﺎﺷر‬ ) T, F ( ‫اﻟﺟواب‬ / F 2 . :‫اﻟﻣﻌﺎدﻻت‬ ‫ﻣن‬ ‫ﻧوﻋﺎن‬ ‫ھﻧﺎك‬ ) A :‫اﻷول‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫اﻟطﻠب‬ (‫)اﻟﮭدف‬ ‫وﺗﺳﻣﻰ‬ ‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬ ،‫اﻟرﺋﯾﺳﯾﺔ‬ :‫اﻟﺛﺎﻧﻲ‬ ‫اﻟﻣﻌﺎدﻻت‬ .‫اﻟﻔرﻋﯾﺔ‬ ) B :‫اﻷول‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫اﻟطﻠب‬ (‫)اﻟﮭدف‬ ‫وﺗﺳﻣﻰ‬ ‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬ ،‫اﻟرﺋﯾﺳﯾﺔ‬ :‫اﻟﺛﺎﻧﻲ‬ ‫اﻟﻣﻌﺎدﻻت‬ .‫اﻟرﺋﯾﺳﯾﺔ‬ ‫اﻟﺟواب‬ / A 3 . ‫اﻟﻣﻼﺣظﺔ‬ ‫اﻷوﻟﻰ‬ :‫اﻟذھﺑﯾﺔ‬ ‫اذا‬ ‫وﺟدت‬ ‫ﻣﺎدة‬ ‫ﻓﻲ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟرﺋﯾﺳﯾﺔ‬ ‫وھﻲ‬ ‫ﻣﺗﻛررة‬ ‫ﻓﻲ‬ ‫اﻛﺛر‬ ‫ﻣن‬ ‫اﻟﺗﻲ‬ ‫اﻟﻣﺎدة‬ ‫اﻟﻰ‬ ‫اﻟﻣﺎدة‬ ‫ھذه‬ ‫ﺗﺟﺎوز‬ ‫ﻓﯾﺗم‬ ‫ﻓرﻋﯾﺔ‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫اﻟرﺋﯾﺳﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﻓﻲ‬ ‫ﺗﻠﯾﮭﺎ‬ ) T, F (
  • 4. ‫اﻟﺟواب‬ / T ( ‫اﻟدرس‬ ‫اﻟﺛﺎﻧﻲ‬ ) ‫ﺣﺳﺎﺑﺎت‬ ‫ﺑﺎﺳﺗﺧدام‬ ‫ﻗﺎﻧون‬ ‫ھﯾس‬ ‫س‬ 1 / ‫إذا‬ ‫أﻋطﯾت‬ ‫اﻟﻣﻌﺎدﻻت‬ ‫اﻟﺣرارﯾﺔ‬ ‫اﻵﺗﯾﺔ‬ ‫ﻋﻧد‬ ‫اﻟظروف‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ) STP :( Δ = 25 KJ 1 ( )𝐹𝑒𝑂(𝑠) + 𝐻2 (𝑔) → 𝐹𝑒(𝑠) + 𝐻2 𝑂(𝑔) 𝐻𝑟 ° Δ = 318 KJ 2 ( )3𝐹𝑒𝑂(𝑠) + 1 2 𝑂2 (𝑔) → 𝐹𝑒3 𝑂4 (𝑠) 𝐻𝑟 ° Δ = - 242 KJ 3 ( )𝐻2 (𝑔) + 1 2 𝑂2 (𝑔) → 𝐻2 𝑂(𝑔) 𝐻𝑟 ° ‫اﺣﺳب‬ Δ ‫ﻟﻠﺗﻔﺎﻋل‬ :‫اﻟﺗﺎﻟﻲ‬ 𝐻𝑟 ° Δ =? 3𝐹𝑒(𝑠) + 4𝐻2 (𝑔) → 𝐹𝑒3 𝑂4 (𝑠) + 4𝐻2 (𝑔) 𝐻𝑟 °
  • 5. /‫اﻟﺣل‬ ‫ﻧﻘﻠب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 1 ( ‫وﻧﺿرﺑﮭﺎ‬ × 3 ‫وﺗﺑﻘﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 2 ( ‫ﻛﻣﺎ‬ ‫ھﻲ‬ ‫وﻧﻘﻠب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 3 :( = -75KJ 1 ( ) 3𝐹𝑒 𝑠 ( ) + 3𝐻2 𝑂 ⟶3𝐹𝑒𝑂 𝑠 ( ) + 3𝐻2 ∆𝐻𝑟 ° 2 ( )𝐹𝑒𝑂 𝑆 ( ) + 1 2 𝑂2 ⟶𝐹𝑒3 𝑂4 𝑆 ( ) ∆𝐻𝑟 ° = − 318𝐾𝐽 3 ( )𝐻2 𝑂 𝑔 ( ) ⟶𝐻2 𝑔 ( ) + 1 2 𝑂2(𝑔) ∆𝐻𝑟 ° = + 242𝐾𝐽 Δ = - 151 KJ2 3𝐹𝑒(𝑠) + 4𝐻2 𝑂(𝑔) → 𝐹𝑒3 𝑂4 + 4𝐻 𝐻𝑟 ° /‫ﻣﻼﺣظﺔ‬ ‫ھﻧﺎ‬ ‫ﻧطﺑق‬ ‫اﻟﻣﻼﺣظﺔ‬ ‫اﻟذھﺑﯾﺔ‬ ‫اﻷوﻟﻰ‬ ‫ﺑﻌدم‬ ‫ﻣوازﻧﺔ‬ ‫ﮫ‬‫ﱠ‬‫ﻧ‬‫ﻷ‬ ‫ﻣﺗﻛرر‬ ‫أﻛﺛر‬ ‫ﻣن‬ ‫ﻣرة‬ ‫ﻓﻲ‬ ‫اﻟﻣﻌﺎدﻻت‬ ،‫اﻟﻔرﻋﯾﺔ‬ 𝐻2 𝑂 ‫وﻛذﻟك‬ ‫ﻧطﺑق‬ ‫اﻟﻣﻼﺣظﺔ‬ ‫اﻟذھﺑﯾﺔ‬ ‫اﻟﺛﺎﻧﯾﺔ‬ ‫ﺑﺿرورة‬ ‫ﻣوازﻧﺔ‬ ‫رﻏم‬ ‫ﺗﻛراره‬ ‫وﻟﻛن‬ ‫ﺑﻌد‬ ‫ﺣﺳﺎب‬ ‫ﻣوﻻﺗﮫ‬ ‫اﻟﺳﺎﺑﻘﺔ‬ ‫ﺑﻌد‬ 𝐻2 ‫اﻟﺗﻐﯾﯾر‬ . ‫س‬ 2 / ‫إذا‬ ‫ﻋﻠﻣت‬ ‫ﱠ‬‫أن‬ ‫اﻧﺛﺎﻟﺑﻲ‬ ‫اﺣﺗراق‬ ّ‫ل‬‫ﻛ‬ ‫ﻣن‬ ‫ﻏﺎز‬ CO ‫و‬ ‫و‬ ‫ﺑوﺣدات‬ KJ/mol ‫ھﻲ‬ ‫ﻋﻠﻰ‬ :‫اﻟﺗواﻟﻲ‬ -) 𝐻2 𝐶𝐻3 𝑂𝐻 727 -/ 286 -/ 284 ،( ‫اﺣﺳب‬ Δ ‫ﺑﺎﺳﺗﺧدام‬ ‫ﻗﺎﻧون‬ ‫ھﯾس‬ ‫ﻟﻠﺗﻔﺎﻋل‬ :‫اﻵﺗﻲ‬ 𝐻𝑟 ° 𝐶𝑂 + 2𝐻2 → 𝐶𝐻3 𝑂𝐻 .‫ﺑﺎﻟﺳؤال‬ ‫ﺗﻌط‬ ‫ﻟم‬ ‫إذا‬ ‫اﻟﻔرﻋﯾﺔ‬ ‫اﻻﺣﺗراق‬ ‫ﻣﻌﺎدﻻت‬ ‫ﻧﻛﺗب‬ ‫ﻣن‬ ‫ﻧﺣن‬ ‫ﺑطرﯾﻘﺔ‬ ‫ﻧﺣﻠﮫ‬ ‫أن‬ ‫ﯾﻣﻛن‬ ‫ﱠ‬‫ﻷن‬ ،‫ھﯾس‬ ‫ﺑطرﯾﻘﺔ‬ ‫اﻟﺳؤال‬ ‫ﺣددﻧﺎ‬ .(‫)اﻟﺳﻣﯾﺷن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻟﺗﻛوﯾن‬ ‫اﻧﺛﺎﻟﺑﻲ‬ = - 284 KJ/mol (1) 𝐶𝑂 + 1 2 𝑂2 → 𝐶𝑂2 ∆𝐻𝑟 ° = - 286 KJ/mol 2 ( )𝐻2 + 1 2 𝑂2 → 𝐻2 𝑂 ∆𝐻𝑟 ° = - 727 KJ/mol 3 ( )𝐶𝐻3 𝑂𝐻 + 3 2 𝑂2 → 𝐶𝑂2 + 2𝐻2 𝑂 ∆𝐻𝑟 ° ‫وﻟﻠﺣﺻول‬ ‫ﻋﻠﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ،‫اﻟرﺋﯾﺳﯾﺔ‬ ‫ﺗﺑﻘﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ) 1 ( ‫ﻛﻣﺎ‬ ،‫ھﻲ‬ ‫وﻧﺿرب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟﻔرﻋﯾﺔ‬ ) 2 ( 2 × ، ‫وﻧﻘﻠب‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟﻔرﻋﯾﺔ‬ ) 3 :( = - 284 KJ/mol (1) 𝐶𝑂 + 1 2 𝑂2 → 𝐶𝑂2 ∆𝐻𝑟 ° = - 572 KJ/mol 2 ( )2𝐻2 + 𝑂2 → 2𝐻2 𝑂 ∆𝐻𝑟 °
  • 6. = + 727 KJ/mol 3 ( )𝐶𝑂2 + 2𝐻2 𝑂 → 𝐶𝐻3 𝑂𝐻 + 3 2 𝑂2 ∆𝐻𝑟 ° Δ = - 129 KJ/mol 𝐶𝑂 + 2𝐻2 → 𝐶𝐻3 𝑂𝐻 𝐻𝑟 ° /‫ﻣﻼﺣظﺔ‬ ‫ﯾﻣﻛن‬ ‫ﺣل‬ ‫اﻟﺳؤال‬ ‫ﺑطرﯾﻘﺔ‬ ‫اﻧﺛﺎﻟﺑﻲ‬ ‫اﻟﺗﻛوﯾن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ) Σ ( ‫ﺑﻌد‬ ‫أن‬ ‫ﻧﺣول‬ ‫ﻗﯾﻣﺔ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﻟﻠﻣﯾﺛﺎﻧول‬ ‫ﻣن‬ ‫اﻹﺷﺎرة‬ ‫ﺑﻘﻠب‬ ‫وذﻟك‬ (‫)اﻟﻣﺎص‬ ‫اﻟﺗﻛوﯾن‬ ‫إﻟﻰ‬ (‫)اﻟﺑﺎﻋث‬ ‫اﻻﺣﺗراق‬ ‫ﻟﻠﻣوﺟب‬ ‫اﻟﺳﺎﻟب‬ ‫ﻣن‬ . ‫س‬ 3 / ‫اﺣﺳب‬ ‫اﻧﺛﺎﻟﺑﻲ‬ ‫اﻟﺗﻛوﯾن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ( )𝐻𝑃𝑂3 = - 180KJ 𝑃4 𝑂10 + 4𝐻𝑁𝑂3 →4𝐻𝑃𝑂3 + 2𝑁2 𝑂5 ∆𝐻𝑟 ° ‫ﻋﻠﻣت‬ ‫اذا‬ Δ = -) 2984 ( KJ/mol 𝐻𝑓 𝑃4 𝑂10 ° Δ = -) 174 ( KJ/mol 𝐻𝑓 𝐻𝑁𝑂3 °
  • 7. Δ =(-43)KJ/mol ?? 𝐻𝑓 𝑁2 𝑂5 ° Δ𝐻𝑟 ° = ∑ 𝑛∆ 𝐻𝑓(𝑃) ° − ∑ 𝑛 ∆𝐻𝑓 𝑅 ( ) ° Δ𝐻𝑟 ° = [4Δ𝐻𝑓(𝐻𝑃𝑂3 ) ° + 2Δ𝐻𝑓(𝑁2 𝑂5 ) ° ] − [Δ𝐻𝑓(𝑃4 𝑂10 ) ° + 4 Δ𝐻𝑓(𝐻𝑁𝑂3 ) ° ] − 180 = 4Δ𝐻𝑓 𝐻𝑃𝑂3 ( ) ° + 2 − 43 ( ) ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ − − 2984 ( ) + 4 − 174 ( ) [ ] − 180 = 4Δ𝐻𝑓 𝐻𝑃𝑂3 ( ) ° − 86 ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ − (− 3680)] - 4∆𝐻𝑓 𝐻𝑃𝑂3 ( ) ° = 3594 + 180⟹4∆𝐻𝑓 𝐻𝑃𝑂3 ( ) ° =− 3594 − 180 ∴∆𝐻𝑓 𝐻𝑃𝑂3 ( ) ° = −3774 4 ⟹∆𝐻𝑓 𝐻𝑃𝑂3 ( ) ° =− 943. 5 𝐾𝐽/𝑚𝑜𝑙 (‫اﻟﺛﺎﻟث‬ ‫)اﻟدرس‬ ‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬
  • 8. : ‫اﻹﻧﺗروﺑﻲ‬ ‫»ھﻲ‬ ‫داﻟﺔ‬ ‫ﺣﺎﻟﺔ‬ ‫ﺛرﻣوداﯾﻧﻣﯾﻛﯾﺔ‬ ‫ﺗﻌﺗﺑر‬ ‫ﻣﻘﯾﺎس‬ ‫ﻟدرﺟﺔ‬ ،‫اﻟﻌﺷواﺋﯾﺔ‬ ‫أو‬ ‫ﻻ‬ ‫اﻧﺗظﺎم‬ ،‫اﻟﻧظﺎم‬ ‫وﯾرﻣز‬ ‫ﻟﮭﺎ‬ ) S ،( ‫وﺗﻘﺎس‬ ‫ﺑوﺣدة‬ ) J/K mol .«( ‫اﻻﻧﺗروﺑﻲ؟‬ ‫اﻟﺣﺎﻟﺔ‬ ‫داﻟﺔ‬ ‫ﻓﺎﺋدة‬ ‫ﻣﺎ‬ /‫ج‬ ‫ﯾﺳﺗﻔﺎد‬ ‫ﻣﻧﮭﺎ‬ ‫ﻟﻠﺗﻧﺑؤ‬ ‫ﺑﺗﻠﻘﺎﺋﯾﺔ‬ ،‫اﻟﺗﻔﺎﻋل‬ ‫ﻓﻛﻠﻣﺎ‬ ‫ﻛﺎن‬ ‫اﻟﻼﻧظﺎم‬ ً‫ﻼ‬‫ﻗﻠﯾ‬ ‫)اﻟﻌﺷواﺋﯾﺔ‬ (‫أﻛﺑر‬ ‫ﻛﺎﻧت‬ ‫ﻗﯾﻣﺔ‬ ‫أﻛﺑر‬ ‫اﻻﻧﺗروﺑﻲ‬ ) ΔS = (+ ‫واﻟﻌﻛس‬ ‫ﺻﺣﯾﺢ‬ :‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻻﻧﺗروﺑﻲ‬ ‫ﺣﺳﺎب‬ ∆𝑆𝑟 о = ∑𝑛 𝑆(𝑃) о − ∑𝑛 𝑆(𝑅) о ‫طﺎﻗﺔ‬ ‫ﻛﺑس‬ ‫اﻟﺣرة‬ ) ΔG :( ‫وﯾﻣﻛن‬ ‫ﺣﺳﺎب‬ ‫اﻟطﺎﻗﺔ‬ ‫اﻟﺣرة‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﺗﻔﺎﻋل‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬ ‫ﻋﻠﻰ‬ ‫اﻟطﺎﻗﺔ‬ ‫اﻟﺣرة‬ ‫ﻟﻠﺗﻛوﯾن‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻣن‬ ‫ﺧﻼل‬ ‫اﺳﺗﺧدام‬ ∆𝐺𝑓 ° (‫)اﻟﺳﻣﯾﺷن‬ ‫اﻟﻣﺟﻣوع‬ ‫ﻗﺎﻧون‬ Δ =𝐺𝑟 ° ∑ 𝑛 ∆𝐺𝑓(𝑃) ° − ∑ 𝑛 ∆𝐺𝑓(𝑅) ° :‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬ ‫ﻟﻧﺎ‬ ‫ﺗﺗﯾﺢ‬ ‫ﺛرﻣوداﯾﻧﻣﯾﻛﯾﺔ‬ ‫ﺣﺎﻟﺔ‬ ‫داﻟﺔ‬ ‫»ھﻲ‬ ‫اﻟﺗﻲ‬ ‫اﻟﻌظﻣﻰ‬ ‫اﻟطﺎﻗﺔ‬ ‫ﺗﻣﺛل‬ ‫وھﻲ‬ ،‫اﻟﺗﻔﺎﻋل‬ ‫ﺑﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺗﻧﺑؤ‬ ‫ﯾﻣﻛن‬ ،‫واﻻﻧﺗروﺑﻲ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﻓﻲ‬ ‫اﻟﺗﻐﯾر‬ ‫ﻗﯾﺎس‬ ‫ﻣن‬ ‫ﻋﻠﯾﮭﺎ‬ ‫اﻟﺣﺻول‬ ‫اﻟﺗﺎﻟﯾﺔ‬ ‫اﻟﻌﻼﻗﺔ‬ ‫ﺑﺣﺳب‬ : ∆𝐺 о = ∆𝐻 о − 𝑇∆𝑆 о ΔG = ‫ﺳﺎﻟﺑﺔ‬ ‫)اﻟﺗﻔﺎﻋل‬ ‫أو‬ ‫اﻟﺗﻐﯾر‬ ‫اﻟﻔﯾزﯾﺎﺋﻲ‬ .(‫ﺗﻠﻘﺎﺋﻲ‬ ΔG = ‫ﻣوﺟﺑﺔ‬ ‫)اﻟﺗﻔﺎﻋل‬ ‫أو‬ ‫اﻟﺗﻐﯾر‬ ‫اﻟﻔﯾزﯾﺎﺋﻲ‬ ‫ﻏﯾر‬ ‫ﺗﻠﻘﺎﺋﻲ‬ ) ΔG = ‫ﺻﻔر‬ ‫)اﻟﺗﻔﺎﻋل‬ ‫أو‬ ‫اﻟﺗﻐﯾر‬ ‫اﻟﻔﯾزﯾﺎﺋﻲ‬ ‫ﻓﻲ‬ ‫ﺣﺎﻟﺔ‬ .(‫اﺗزان‬ ‫ﻣﻼﺣظﺎت‬ ‫ﻣﮭﻣﺔ‬ : 1 . Δ ‫ﻟﻠﻌﻧﺎﺻر‬ ‫اﻟﺣرة‬ ‫ﺑﺄﺛﺑت‬ ‫ﺻورھﺎ‬ = .‫ﺻﻔر‬ 𝐻𝑓 ° ‫ﻣﺛﺎل‬ / / / / :( ... ‫اﻟﺦ‬ .( 𝐴𝑙(𝑠) 𝐶𝑙2 (𝑔) 𝑁2 (𝑔) 𝑂2 (𝑔) 𝐻2 (𝑔)
  • 9. 2 . ‫أﻓﺿل‬ ‫طرﯾﻘﺔ‬ ‫ﻻﺳﺗﺧدام‬ ‫اﻟﺳﻣﯾﺷن‬ ‫ھو‬ ‫إﻧﮭﺎء‬ ‫ﻧﺎﺗﺞ‬ ّ‫ل‬‫ﻛ‬ ‫طرف‬ ‫ﺑدﻗﺔ‬ ‫ﺛم‬ ‫ﻧﻘوم‬ ‫ﺑﻌﻣﻠﯾﺔ‬ ‫طرح‬ ‫اﻟطرف‬ ‫اﻷول‬ ‫ﻣن‬ .‫اﻟﺛﺎﻧﻲ‬ 3 . ‫رﺑﻣﺎ‬ ‫ﺗﻛون‬ Δ ‫ﻣﻌﻠوﻣﺔ‬ ‫و‬ Δ ‫ﻟﻣﻌظم‬ ‫ﻣواد‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﻣﻌﻠوﻣﺔ‬ ‫وﯾﻛون‬ ‫اﻟﻣطﻠوب‬ Δ ‫ﻟﻣﺎدة‬ ‫ﻣﺟﮭوﻟﺔ‬ .‫واﺣدة‬ 𝐺𝑟 ° 𝐺𝑓 ° 𝐺𝑓 ° 4 . ‫إذا‬ ‫ﻛﺎن‬ ‫اﻟطرف‬ ‫اﻟﺛﺎﻧﻲ‬ ‫ﻧﺎﺗﺟﮫ‬ ‫ﺳﺎﻟب‬ ‫ﻓﺗﺻﺑﺢ‬ ‫اﻟﻌﻣﻠﯾﺔ‬ :‫اﻟﺣﺳﺎﺑﯾﺔ‬ ‫اﻟﺛﺎﻧﻲ‬ ‫اﻟطرف‬ + ‫اﻷول‬ ‫اﻟطرف‬ ‫س‬ 1 / ‫ﻋرف‬ ‫طﺎﻗﺔ‬ ‫ﻛﺑس‬ ‫اﻟﺣرة‬ ‫ﻟﻠﺗﻛوﯾن‬ ،‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫وﻣﺎ‬ ‫ھﻲ‬ ‫وﺣداﺗﮭﺎ؟‬ »/ ‫اﻟﺟواب‬ ‫ﺗﻛوﯾن‬ ‫ﻋﻧد‬ ‫اﻟﺣرة‬ ‫اﻟطﺎﻗﺔ‬ ‫ﻓﻲ‬ ‫اﻟﺗﻐﯾﯾر‬ ‫ﻣﻘدار‬ ‫ھﻲ‬ ‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ‫ﻋﻧﺎﺻرھﺎ‬ ‫ﻣن‬ ‫ﻣرﻛب‬ ‫أي‬ ‫ﻣن‬ ‫واﺣد‬ ‫ﻣول‬ ،‫ﺻورة‬ ‫وﻋﻧد‬ ‫اﻟظروف‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ) 1 atm/25 ( ‫وﯾرﻣز‬ ‫ﻟﮭﺎ‬ ) ( ‫ووﺣداﺗﮭﺎ‬ ) KJ/mol)» s ℃ 𝐷𝐺𝑓 ° ‫ﻣﺛﺎل‬ 2 / ‫اﺣﺳب‬ ‫طﺎﻗﺔ‬ ‫ﻛﺑس‬ ‫اﻟﺣرة‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺗﺎﻟﻲ‬ ‫ﻋﻧد‬ ‫اﻟظروف‬ ،‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﺛم‬ ‫ن‬ّ‫ﯾ‬‫ﺑ‬ ‫ھل‬ ‫ﯾﺟري‬ ‫اﻟﺗﻔﺎﻋل‬ ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬ ‫أم‬ :‫اﻟظروف‬ ‫ھذه‬ ‫ﻋﻧد‬ ،‫ﻻ‬ 2𝐶6 𝐻6 (𝐿) + 15𝑂2 (𝑔) → 12𝐶𝑂2 (𝑔) + 6𝐻2 𝑂(𝐿) :‫ﻋﻠﻣت‬ ‫إذا‬ = (- 394) KJ/mol, ∆𝐺𝑓𝐶𝑂2 ° = (- 237) KJ/mol ∆𝐺𝑓𝐻2 𝑂 ° = (173) KJ/mol ∆𝐺𝑓𝐶6 𝐻6 ° /‫اﻟﺣل‬ Δ = 𝐺𝑟 ° ∑ 𝑛 ∆𝐺𝑓(𝑃) ° − ∑ 𝑛 ∆𝐺𝑓(𝑅) ° Δ = ] 12 + 6 [ - ] + 15 [ 𝐺𝑟 ° ∆𝐺𝑓𝐶𝑂2 ° ∆𝐺𝑓𝐻2 𝑂 ° 2∆𝐺𝑓𝐶6 𝐻6 ° ∆𝐺𝑓𝑂2 ° = Δ = [(- 4728) + (- 1422)] - (346) 𝐺𝑟 ° Δ = - 6496 KJ/mol = ‫)ﺳﺎﻟﺒﺔ‬ , ( ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ ‫ﱠ‬‫ﻷن‬ ∴ 𝐺𝑟 ° ∆𝐺°𝑟
  • 10. ‫ﺗﻣرﯾن‬ 1 / ‫اﺣﺳب‬ ‫طﺎﻗﺔ‬ ‫ﻛﺑس‬ ‫اﻟﺣرة‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺗﺎﻟﻲ‬ ‫ﻋﻧد‬ ‫اﻟظروف‬ ،‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ن‬ّ‫ﯾ‬‫وﺑ‬ ‫ھل‬ ‫ﯾﺟري‬ ‫اﻟﺗﻔﺎﻋل‬ ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬ ‫أم‬ ‫ﻻ؟‬ 2𝑁𝑂(𝑔) + 𝑂2 (𝑔) →2𝑁𝑂2 (𝑔) :‫ﻋﻠﻣت‬ ‫إذا‬ ∆𝐺𝑓𝑁𝑂 ° = 87 𝐾𝐽 𝑚𝑜𝑙 ∆𝐺𝑓𝑁𝑂2 ° = 52 𝐾𝐽 𝑚𝑜𝑙 /‫اﻟﺣل‬ Δ = ] 2 ) [( - ] 2 ) ( + [ 𝐺𝑟 ° ∆𝐺𝑓𝑁𝑂2 ° ∆𝐺𝑓𝑁𝑂 ° ∆𝐺𝑓𝑂2 ° = ] 2 ) 52 [( - ] 2 ) 87 ( + 0 [ Δ = (104) - (174) ⇒ Δ = - 70 KJ/mol ‫ﺗﻠﻘﺎﺋﻲ‬ ∴ 𝐺𝑟 ° 𝐺𝑟 ° ‫ﻣﻼﺣظﺔ‬ / ‫ﻟﻠﻌﻨﺎﺻﺮ‬ ‫اﻟﺤﺮة‬ ‫ﺑﺎﺛﺒﺖ‬ ‫ﺻﻮرة‬ = ‫ﺻﻔﺮ‬ ∆𝐺 °
  • 11. ‫اﻟﺛﺎﻟث‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬ 1 . Δ ‫ﻟﻠﻌﻧﺎﺻر‬ ‫اﻟﺣرة‬ ‫ﺑﺄﺛﺑت‬ ‫ﺻورھﺎ‬ = .‫ﺻﻔر‬ 𝐺𝑓 ° ) T, F ( ‫اﻟﺟواب‬ / T 2 . ‫أﻓﺿل‬ ‫طرﯾﻘﺔ‬ ‫ﻻﺳﺗﺧدام‬ ‫اﻟﺳﻣﯾﺷن‬ ‫ھو‬ ‫إﻧﮭﺎء‬ ‫ﻧﺎﺗﺞ‬ ّ‫ل‬‫ﻛ‬ ‫طرف‬ ‫ﺑدﻗﺔ‬ ‫ﺛم‬ ‫ﻧﻘوم‬ ‫ﺑﻌﻣﻠﯾﺔ‬ ‫ﺟﻣﻊ‬ .‫اﻟﺛﺎﻧﻲ‬ ‫ﻣن‬ ‫اﻷول‬ ‫اﻟطرف‬ ) T, F ( ‫اﻟﺟواب‬ / F 3 . ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫ﻟﻠﺗﻛوﯾن‬ ‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬ : ) A ‫ھﻲ‬ ‫ﻣﻘدار‬ ‫اﻟﺗﻐﯾﯾر‬ ‫ﻓﻲ‬ ‫اﻟطﺎﻗﺔ‬ ‫اﻟﺣرة‬ ‫ﻋﻧد‬ ‫ﺗﻛوﯾن‬ ‫ﻣول‬ ‫واﺣد‬ ‫ﻣن‬ ‫أي‬ ‫ﻣرﻛب‬ ‫ﻣن‬ ‫ﻋﻧﺎﺻرھﺎ‬ ،‫ﺻورة‬ ‫ﺑﺄﺛﺑت‬ ‫اﻷﺳﺎﺳﯾﺔ‬ ) B ‫اﻟظروف‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ) 1 atm/50 ( ‫وﯾرﻣز‬ ‫ﻟﮭﺎ‬ ) ( ‫ووﺣداﺗﮭﺎ‬ ) KJ/mol .( ∆𝐺𝑓 ° ) C ‫اﻟظروف‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ) 1 atm/25 ( ‫وﯾرﻣز‬ ‫ﻟﮭﺎ‬ ) ( ‫ووﺣداﺗﮭﺎ‬ ) KJ/mol .( ∆𝐺𝑓 ° ‫اﻟﺟواب‬ / A & C
  • 12. ( ‫اﻟراﺑﻊ‬ ‫)اﻟدرس‬ ‫اﻟﺗﻔﺎﻋﻼت‬ ‫ﺳﯾر‬ ‫وﺗﺟﺎه‬ ‫ﻛﺑس‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬ ‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬ ‫اﻟﻛﯾﻣﯾﺎﺋﯾﺔ‬ ‫اﻟﺗﻔﺎﻋﻼت‬ ‫ﺳﯾر‬ ‫واﺗﺟﺎه‬ ‫ﻛﺑس‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬ ∆𝐺𝑟 ° = ∆𝐻𝑟 ° − 𝑇∆𝑆𝑟 ‫ﺳؤال‬ / ‫اﻟﺗﻔﺎﻋل؟‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫ﯾﺿﻣﻧﺎن‬ ‫ﻋﺎﻣﻠﯾن‬ ‫أﻛﺛر‬ ‫ھﻣﺎ‬ ‫ﻣﺎ‬ /‫ج‬ ‫ﱠ‬‫إن‬ ‫اﻟﺘﻐﯿﺮ‬ ‫ﻓﻲ‬ ‫اﻟﻄﺎﻗﺔ‬ ‫اﻟﺤﺮة‬ ) Δ ( ‫ﯾﺘﻀﻤﻦ‬ ‫ﻋﺎﻣﻠﯿﻦ‬ ‫ﻣﮭﻤﯿﻦ‬ ‫ﯾﺆﺛﺮان‬ ‫ﻋﻠﻰ‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ،‫اﻟﺘﻔﺎﻋﻞ‬ :‫وھﻤﺎ‬ 𝐺𝑟 ° 1 . 𝐷𝐻𝑟 о 2 . 𝐷𝑆𝑟 ° ‫واذا‬ ‫ﻛﺎﻧﺖ‬ ‫اﺷﺎرة‬ ‫و‬ ‫ﻣﺘﺸﺎﺑﮭﺔ‬ ‫ﺗﻜﻮن‬ ‫درﺟﺔ‬ ‫اﻟﺤﺮارة‬ ‫ھﻲ‬ ‫اﻟﻤﺘﺤﻜﻢ‬ ‫اﻟﺮﺋﯿﺴﻲ‬ ‫ﻓﻲ‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ 𝐷𝐻𝑟 о 𝐷𝑆𝑟 о /‫ﻋﻠل‬ ‫ﺗﻠﻘﺎﺋﯾﺔ؟‬ ‫أﻛﺛر‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻛﺎن‬ ‫ﻋﺎﻟﯾﺔ‬ ‫اﻻﻧﺗروﺑﻲ‬ ‫ﻛﺎﻧت‬ ‫ﻛﻠﻣﺎ‬ /‫ج‬ (∆𝐺°𝑟 = ∆𝐻°𝑟 − 𝑇∆𝑆°𝑟 ) ‫ﱠ‬‫ﻷن‬ ‫اﻻﻧﺘﺮوﺑﻲ‬ ‫ﺗﻘﻊ‬ ‫ﺿﻤﻦ‬ ‫اﻟﺤﺪ‬ ) ‫اﻟﺴﺎﻟﺐ‬ ‫وﺑﺎﻟﺘﺎﻟﻲ‬ ‫ﻛﻠﻤﺎ‬ ‫ﺗﻜﻮن‬ ‫ﻗﯿﻤﺔ‬ ‫ھﺬا‬ ‫اﻟﺤﺪ‬ ‫أﻋﻠﻰ‬ ‫ﻣﻦ‬ ) > 𝑇∆𝑆°𝑟 ) ∆𝐻°𝑟 ∆𝐻°𝑟 ( ‫ﻛﺎﻧﺖ‬ ‫ﻗﯿﻤﺔ‬ = ،‫ﺳﺎﻟﺒﺔ‬ ‫وﺑﺎﻟﺘﺎﻟﻲ‬ ‫ﯾﻜﻮن‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ . 𝑇∆𝑆°𝑟 𝐷𝐺°𝑟 ‫ﻣﻼﺣظﺔ‬ / ‫ﺣﯿﻨﻤﺎ‬ ‫ﺗﻜﻮن‬ ‫إﺷﺎرات‬ ) ΔH, ΔS ( ‫ﻣﺨﺘﻠﻔﺔ‬ ‫ﻓﻠﯿﺲ‬ ‫ھﻨﺎك‬ ‫ﺗﺄﺛﯿﺮ‬ ‫ﻟﺪرﺟﺔ‬ ،‫اﻟﺤﺮارة‬ ‫وﻻﺣﻆ‬ ‫ﱠ‬‫أن‬ ‫إﺷﺎرة‬ ) ΔH ( ‫ﺗﺸﺎﺑﮫ‬ ‫إﺷﺎرة‬ ) ΔG ( ‫ﻓﻲ‬ .‫اﻟﻐﺎﻟﺐ‬
  • 13. :‫ﻣﮭﻣﺔ‬ ‫ﻣﻼﺣظﺎت‬ ΔG .1 = ‫ﺳﺎﻟﺒﺔ‬ (-) ‫اﻟﺘﻔﺎﻋﻞ‬ ،‫ﺗﻠﻘﺎﺋﻲ‬ ΔG = ‫ﻣﻮﺟﺒﺔ‬ (+) ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻏﯿﺮ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ 2 . :‫ﻋﻤﻠﯿﺎت‬ ‫)اﻻﻧﺼﮭﺎر‬ / ‫اﻟﺘﺒﺨﺮ‬ (‫)اﻟﻐﻠﯿﺎن‬ / ‫اﻟﺘﺴﺎﻣﻲ‬ (... ΔS = (+) ‫ﺗﺰداد‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ ΔH = (+) ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻣﺎص‬ 3 . ‫ﻋﻤﻠﯿﺎت‬ ‫)اﻻﻧﺠﻤﺎد‬ ‫)اﻟﺘﺒﻠﻮر‬ / ‫اﻟﺘﻜﺜﯿﻒ‬ (‫)اﻟﻨﺪى‬ / ‫اﻟﺘﺼﻠﺐ‬ (... ΔS = (-) ‫ﺗﻘﻞ‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ ΔH = (-) ‫ﺑﺎﻋﺚ‬ ‫ﻟﻠﺤﺮارة‬ 4 . ‫ﺣﯿﻨﻤﺎ‬ :‫ﯾﻘﻮل‬ ‫)ﯾﺴﺒﺐ‬ ‫اﻧﺨﻔﺎض‬ ‫درﺟﺔ‬ ‫ﺣﺮارة‬ :(‫اﻟﻤﺤﻠﻮل‬ ‫ﺑﺎﻋﺜﺔ‬ ‫واﻟﻌﻜﺲ‬ ‫ﻣﺎﺻﺔ‬ ‫اﻟﻌﻤﻠﯿﺔ‬ ) ΔH > TΔS ( 5 . ‫ذوﺑﺎن‬ ‫ﺻﻠﺐ‬ ‫أو‬ ،‫ﺳﺎﺋﻞ‬ ‫ﺗﺰداد‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ +) = ΔS ( ‫وﻋﻠﻰ‬ ‫اﻷﻏﻠﺐ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻣﺎص‬ +) = ΔH ( 6 . ‫ذوﺑﺎن‬ ،‫ﻏﺎز‬ ‫ﺗﻘﻞ‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ -) = ΔS ،( ‫وھﻲ‬ :‫ﻋﻤﻠﯿﺎت‬ ‫ﺑﺎﻋﺜﺔ‬ -) = ΔH ( 7 . ‫ﻋﻤﻠﯿﺎت‬ ‫)اﻟﺘﺤﻠﻞ‬ / ‫اﻟﺘﻔﻜﻚ‬ / :(‫اﻟﺘﺄﯾﻦ‬ ‫)ﺗﺰداد‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ +) = ΔS ( ‫واﻟﺘﻔﺎﻋﻞ‬ ‫ﻣﺎص‬ +) = ΔH ( 8 . :‫ﻋﻤﻠﯿﺎت‬ ‫)اﻻﺗﺤﺎد‬ / ‫اﻻﻧﺪﻣﺎج‬ :(... ‫ﺗﻘﻞ‬ ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ -) = ΔH ( 9 . ‫أھم‬ :‫ﻣﻼﺣظﺔ‬ ‫)إن‬ ‫ﻛﺎﻧﺖ‬ ‫اﻟﻌﺒﺎرات‬ ‫ﻣﻨﻔﯿﺔ‬ ‫ﻓﺎﻟﺘﻔﺎﻋﻞ‬ ‫ﻏﯿﺮ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ +) = ΔG ،( ‫وﻧﺮﻓﻊ‬ ‫اﻟﻨﻔﻲ‬ ً‫ﺎ‬‫ﻣﺆﻗﺘ‬ ‫ﺛﻢ‬ ‫ﻧﺤﻞ‬ ‫اﻟﻤﺴﺄﻟﺔ‬ ‫ﻋﻠﻰ‬ .(‫اﻟﻘﺎدﻣﺔ‬ ‫اﻟﻤﺴﺎﺋﻞ‬ ‫ﻣﻦ‬ ‫ذﻟﻚ‬ ‫ﺳﯿﺘﻮﺿﺢ‬ ‫ﻛﻤﺎ‬ ،‫ﻛﺒﺲ‬ ‫ﻋﻼﻗﺔ‬ ‫ﺿﻮء‬
  • 14. ‫اﻟراﺑﻊ‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬ 1 . ‫اﻟﺗﻔﺎﻋل‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫ﯾﺿﻣﻧﺎن‬ ‫ﻋﺎﻣﻠﯾن‬ ‫أﻛﺛر‬ ‫ھﻣﺎ‬ ‫ﻣﺎ‬ ) A Δ𝐻°𝑟 & Δ𝐶°𝑟 ) B ∆𝐻°𝑟 & Δ𝑆°𝑟 ) C ∆𝐺°𝑟 & Δ𝑆°𝑟 (‫)ﺧﯾﺎرات‬ ‫اﻟﺳؤال‬ ‫ﻧوع‬ ‫اﻟﺟواب‬ / B 2 . ‫اﻟﺗﺻﻠب‬ / (‫)اﻟﻧدى‬ ‫اﻟﺗﻛﺛﯾف‬ / ‫)اﻟﺗﺑﻠور‬ ‫)اﻻﻧﺟﻣﺎد‬ ‫ﻋﻣﻠﯾﺎت‬ (... ΔS = (+) ‫ﺗزداد‬ ‫اﻟﻌﺷواﺋﯾﺔ‬ ΔH = (-) ‫ﺑﺎﻋث‬ ‫ﻟﻠﺣرارة‬ ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / F 3 . ،‫ﻏﺎز‬ ‫ذوﺑﺎن‬ ‫ﺗﻘل‬ ‫اﻟﻌﺷواﺋﯾﺔ‬ -) = ΔS ،( ‫وھﻲ‬ :‫ﻋﻣﻠﯾﺎت‬ ‫ﺑﺎﻋﺛﺔ‬ -) = ΔH ( ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / T (‫اﻟﺧﺎﻣس‬ ‫)اﻟدرس‬ ‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫وﻓق‬ ‫ﺗﻌﺎﻟﯾل‬ ‫ﻋﻠل‬ ‫ﻣﺎ‬ ‫ﯾﺄﺗﻲ‬ ‫ﻋﻠﻰ‬ ‫وﻓق‬ ‫ﻋﻼﻗﺔ‬ :‫ﻛﺑس‬ ‫س‬/ 3
  • 15. 1 . ‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺟﻠﯾد‬ ‫اﻧﺻﮭﺎر‬ ‫ﻋﻣﻠﯾﺔ‬ /‫ج‬ - ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ΔG = ‫ﺳﺎﻟﺒﺔ‬ ‫)اﻟﺘﻔﺎﻋﻞ‬ (‫ﺗﻠﻘﺎﺋﻲ‬ - ‫اﻧﺼﮭﺎر‬ ΔS = ‫ﻣﻮﺟﺒﺔ‬ ‫)ﺗﺰداد‬ (‫اﻟﻌﺸﻮاﺋﯿﺔ‬ - ‫اﻟﻌﻤﻠﯿﺔ‬ ‫ﻣﺎﺻﺔ‬ ΔH = ‫ﻣﻮﺟﺒﺔ‬ ΔG = ΔH - TΔS + (-) + = - ΔH < TΔS 2 . ‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫اﻷوﻟﯾﺔ‬ ‫ﻋﻧﺎﺻره‬ ‫إﻟﻰ‬ ‫اﻟﻣﺎء‬ ‫ﯾﺗﺣﻠل‬ ‫ﻻ‬ /‫ج‬ - ‫اﻟﻌﻤﻠﯿﺔ‬ ‫ﻏﯿﺮ‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ΔG = ‫ﻣﻮﺟﺒﺔ‬ - ‫ﯾﺘﺤﻠﻞ‬ ΔS = ‫ﻣﻮﺟﺒﺔ‬ ‫)ﺗﺰداد‬ (‫اﻟﻌﺸﻮاﺋﯿﺔ‬ - ‫اﻟﻌﻤﻠﯿﺔ‬ ‫ﻣﺎﺻﺔ‬ ‫ﻟﻠﺤﺮارة‬ ΔH = ‫ﻣﻮﺟﺒﺔ‬ ΔG = ΔH - TΔS + (-) + = + ΔH > TΔS 3 . ‫ﯾذوب‬ ‫ﻏﺎز‬ ‫ﻓﻲ‬ ‫اﻟﻣﺎء‬ ‫وﯾﺑﻌث‬ ‫ﺣرارة‬ ‫ﻋﺎﻟﯾﺔ‬ ‫؟‬ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯾ‬ 𝑆𝑂2 /‫ج‬ ‫اﻟﻌﻤﻠﯿﺔ‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ΔG = ‫ﻣﻮﺟﺒﺔ‬ ‫ذوﺑﺎن‬ ‫ﻏﺎز‬ ΔS = ‫ﺳﺎﻟﺒﺔ‬ ‫)ﺗﻘﻞ‬ (‫اﻟﻌﺸﻮاﺋﯿﺔ‬ ‫اﻟﻌﻤﻠﯿﺔ‬ ‫ﺑﺎﻋﺜﺔ‬ ΔH = ‫ﺳﺎﻟﺒﺔ‬ ΔG = ΔH - TΔS - (+) - = -
  • 17. 1 ‫ﻋﻨﺪﻣﺎ‬- ‫ﺗﻜﻮن‬ ‫اﺷﺎرة‬ ) ( ‫ﻣﺘﺸﺎﺑﮭﺔ‬ ∆𝐻, ∆𝑆 a) ∆𝐻 =− ∆𝑆 =− ∆𝐺 = ∆𝐻 − 𝑇∆𝑆 − ( ) − − ( ) − ( ) (+) ‫ھﻨﺎ‬ ‫ﯾﻜﻮن‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ ‫ﻋﻨﺪﻣﺎ‬ ‫ﺗﻜﻮن‬ (‫)ﺗﺒﺮﯾﺪ‬ ∆𝐻 > 𝑇∆𝑆 b) ∆𝐻 =+ ∆𝑆 =+ ∆𝐺 = ∆𝐻 − 𝑇∆𝑆 + ( ) − + ( ) + ( ) (−) ‫ھﻨﺎ‬ ‫ﯾﻜﻮن‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ ‫ﻋﻨﺪﻣﺎ‬ ‫ﺗﻜﻮن‬ (‫)ﺗﺴﺨﯿﻦ‬ 𝑇∆𝑆 > ∆𝐻 ‫اﻟﺧﺎﻣس‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
  • 18. 1 . ‫؟‬ ‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ‫اﻟﺟﻠﯾد‬ ‫اﻧﺻﮭﺎر‬ ‫ﻋﻣﻠﯾﺔ‬ ) A ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ΔG = ‫ﺳﺎﻟﺑﺔ‬ ‫)اﻟﺗﻔﺎﻋل‬ (‫ﺗﻠﻘﺎﺋﻲ‬ - ‫اﻧﺻﮭﺎر‬ ΔS = ‫ﻣوﺟﺑﺔ‬ ‫)ﺗزداد‬ (‫اﻟﻌﺷواﺋﯾﺔ‬ - ‫اﻟﻌﻣﻠﯾﺔ‬ ‫ﻣﺎﺻﺔ‬ ΔH = ‫ﺳﺎﻟﺑﺔ‬ ΔG = ΔH - TΔS + (-) + = - ΔH > TΔS ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / F 2 . ‫اﻻﻋﺗﯾﺎدﯾﺔ‬ ‫ﺑﺎﻟظروف‬ ‫اﻷوﻟﯾﺔ‬ ‫ﻋﻧﺎﺻره‬ ‫إﻟﻰ‬ ‫اﻟﻣﺎء‬ ‫ﯾﺗﺣﻠل‬ ‫ﻻ‬ :‫ﺑﺳﺑب‬ ‫وذﻟك‬ ) A ‫اﻟﻌﻣﻠﯾﺔ‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ΔG = ‫ﻣوﺟﺑﺔ‬ - ‫ﯾﺗﺣﻠل‬ ΔS = ‫ﻣوﺟﺑﺔ‬ ‫)ﺗزداد‬ (‫اﻟﻌﺷواﺋﯾﺔ‬ ) B ‫اﻟﻌﻣﻠﯾﺔ‬ ‫ﻏﯾر‬ ‫ﺗﻠﻘﺎﺋﯾﺔ‬ ΔG = ‫ﻣوﺟﺑﺔ‬ - ‫ﯾﺗﺣﻠل‬ ΔS = ‫ﻣوﺟﺑﺔ‬ ‫)ﺗزداد‬ (‫اﻟﻌﺷواﺋﯾﺔ‬ - ‫اﻟﻌﻣﻠﯾﺔ‬ ‫ﻣﺎﺻﺔ‬ ‫ﻟﻠﺣرارة‬ ΔH = ‫ﻣوﺟﺑﺔ‬ ( ‫اﻟﺳﺎدس‬ ‫)اﻟدرس‬ ‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫ﺣﺳﺎﺑﺎت‬ :‫ﻛﺑس‬ ‫ﻋﻼﻗﺔ‬ ‫ﺣﺳﺎﺑﺎت‬
  • 19. ‫ﯾﻤﻜﻦ‬ ‫اﺳﺘﺨﺪام‬ ‫ﻋﻼﻗﺔ‬ ‫ﻛﺒﺲ‬ ‫ﻟﺤﺴﺎب‬ ‫ﻗﯿﻤﺔ‬ ‫اﻟﻄﺎﻗﺔ‬ ‫اﻟﺤﺮة‬ Δ ‫اﻟﻘﯿﺎﺳﯿﺔ‬ ‫وﺑﺎﻟﺘﺎﻟﻲ‬ ‫ﻣﻌﺮﻓﺔ‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ‫أو‬ ‫ﻋﺪم‬ ‫ﺗﻠﻘﺎﺋﯿﺔ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫وذﻟﻚ‬ 𝐺𝑟 ° ‫إذا‬ ‫ﺗﻢ‬ ‫ﻗﯿﺎس‬ ‫ﻗﯿﻢ‬ Δ ‫و‬ ، ‫ﻋﻨﺪ‬ ‫اﻟﻈﺮوف‬ ‫اﻟﻘﯿﺎﺳﯿﺔ‬ ) 1 atm/25 ( ، ‫وذﻟﻚ‬ ‫ﻣﻦ‬ ‫ﺧﻼل‬ ‫اﻟﻌﻼﻗﺔ‬ :‫اﻟﺘﺎﻟﯿﺔ‬ 𝐻𝑟 ° ∆𝑆𝑟 ° ℃ ∆𝐺𝑟 ° = ∆𝐻𝑟 ° − 𝑇∆𝑆𝑟 ° ‫ﻣﻼﺣظﺔ‬ 1 / ‫ﯾﺠﺐ‬ ‫اﻟﺘﻤﯿﯿﺰ‬ ‫ﺑﯿﻦ‬ Δ ‫و‬ ‫وﺑﯿﻦ‬ Δ ‫و‬ Δ . 𝐺𝑟 ° ∆𝐺𝑓 ° 𝐻𝑟 ° 𝐻𝑓 ° ‫ﻣﻼﺣظﺔ‬ 2 / ‫ﻗﯿﻢ‬ ‫اﻻﻧﺜﺎﻟﺒﻲ‬ ‫واﻟﻄﺎﻗﺔ‬ ‫اﻟﺤﺮة‬ ‫ﻟﻠﻌﻨﺎﺻﺮ‬ ‫اﻟﺤﺮة‬ ‫ﺑﺄﺛﺒﺖ‬ ‫ﺻﻮرة‬ ‫ﺗﺴﺎوي‬ ‫ﺻﻔﺮ‬ ‫ﻣﻼﺣظﺔ‬ 3 / ‫ﯾﺠﺐ‬ ‫ﺗﻮﺣﯿﺪ‬ ‫وﺣﺪﺗﻲ‬ ‫و‬ Δ ‫ﻗﺒﻞ‬ ‫ﺗﻄﺒﯿﻖ‬ ‫ﻋﻼﻗﺔ‬ .‫ﻛﺒﺲ‬ ∆𝑆𝑟 ° 𝐺𝑟 ° ‫ﻣﻼﺣظﺔ‬ 4 / ‫اﻟﻌﺸﻮاﺋﯿﺔ‬ (‫)اﻻﻧﺘﺮوﺑﻲ‬ ‫ﻟﻠﺠﺰﯾﺌﺎت‬ ‫ﺗﻌﺘﻤﺪ‬ ‫ﻋﻠﻰ‬ ‫اﻟﻄﺎﻗﺔ‬ ،‫اﻟﺤﺮﻛﯿﺔ‬ ‫وھﻲ‬ ‫ﺣﺮﻛﺎت‬ ‫ﺻﻐﯿﺮة‬ ‫ﺑﺎﻟﻨﺴﺒﺔ‬ ‫ﻟﻘﯿﻢ‬ ‫اﻻﻧﺜﺎﻟﺒﻲ‬ ‫واﻟﻄﺎﻗﺔ‬ ‫اﻟﺤﺮة‬ ‫ﻟﺬﻟﻚ‬ ‫ﺗﻜﻮن‬ ‫وﺣﺪة‬ ΔS ‫ﺻﻐﯿﺮة‬ ‫ﺑﺎﻟﺠﻮل‬ ) J ( ‫ووﺣﺪات‬ ΔH ‫و‬ ΔG ‫ﻛﺒﯿﺮة‬ ‫ﺑﺎﻟـ‬ ) KJ .( ‫س‬ 4 / ‫ﺟد‬ ‫ﻗﯾﻣﺔ‬ ) ( ‫ﻟﻠﺗﻔﺎﻋل‬ :‫اﻟﺗﺎﻟﻲ‬ ∆𝐺°𝑟 2𝐶𝑂(𝑔) + 𝑂2 (𝑔) → 2𝐶𝑂2 (𝑔) ‫اﻟﻣﻌﻠوﻣﺎت‬ ‫أﻋطﯾت‬ ‫إذا‬ ‫اﻟﻘﯾﺎﺳﯾﺔ‬ ‫اﻟظروف‬ ‫ﺗﺣت‬ ‫ﯾﺟري‬ ‫اﻟذي‬ :‫اﻵﺗﯾﺔ‬ Δ = -) 110.5 ( KJ/mol , 𝐻𝑓𝐶𝑂 ° Δ = -) 393.5 ( KJ/mol 𝐻𝑓𝐶𝑂2 ° = 198 J/K mol , 𝑆𝐶𝑂 ° = 214 J/K mol , 𝑆𝐶𝑂2 ° = 205 J/K mol 𝑆𝑂2 ° /‫اﻟﺣل‬ 1 - Δ 𝐻𝑟 ° = 2∆𝐻𝑓𝐶𝑂2 ° ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ − 2∆𝐻𝑓𝐶𝑂 ° ( )+ ∆𝐻𝑓𝑂2 ° ( ) ⎡ ⎢ ⎣ ⎤ ⎥ ⎦
  • 20. Δ 𝐻𝑟 ° = 2 × − 393. 5 ( ) [ ] − 2 × − 110. 5 ( ) + 0 [ ] Δ 𝐻𝑟 ° = − 787 ( ) + 221 ( ) ∆𝐻𝑟 ° = − 566 𝐾𝐽/𝑚𝑜𝑙 2. ∆𝑆𝑟 ° = 2𝑆𝐶𝑂2 ° ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ − 2𝑆𝐶𝑂 ° + 𝑆𝑂2 ° ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ ∆𝑆𝑟 ° = [2 × 214] − [2 × 198) + 205] ∆𝑆𝑟 ° = − 173 𝐽/𝐾 𝑚𝑜𝑙 = -0.173 KJ/K mol ‫ﻧﻮﺣﺪ‬ ‫اﻟﻮﺣﺪات‬ ∆𝑆𝑟 ° = −173 1000 3. Δ ∴ 𝐺𝑟 ° = ∆𝐻𝑟 ° − 𝑇 ∆𝑆𝑟 ° , 𝑇𝑘 = 𝑡℃ + 273 𝑇𝑘 = 25 + 273 = 298𝐾 = -566 - (298) (-0.173) Δ ∴ 𝐺𝑟 ° = − 514. 446 𝐾𝐽 𝑚𝑜𝑙 (‫ﺗﻠﻘﺎﺋﻲ‬ ‫)اﻟﺘﻔﺎﻋﻞ‬ ‫س‬ 5 / ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺗﺎﻟﻲ‬ 2𝐻2 𝑔 ( ) + 𝑂2 (𝑔) → 2𝐻2 𝑂(𝑔) (J/K.mol) ‫ﻟﻠﺗﻔﺎﻋل‬ ‫ﺑوﺣدة‬ ‫اﺣﺳب‬ ‫ﻗﯾﻣﺔ‬ ∆𝑆𝑟 ° :‫ﻋﻠﻣت‬ ‫إذا‬ Δ𝐻𝑓𝐻2 𝑂 ° = − 242 ( )𝐾𝐽/𝑚𝑜𝑙) Δ𝐺𝑓𝐻2 𝑂 ° = − 228 ( )𝐾𝐽/𝑚𝑜𝑙)
  • 21. /‫اﻟﺣل‬ Δ 𝐻𝑟 ° = ∑ 𝑛∆𝐻𝑓(𝑃) ° − ∑ 𝑛 ∆𝐻𝑓(𝑅) ° = ] 2Δ [𝐻𝑓𝐻2 𝑂 ° − [2∆𝐻𝑓𝐻2 ° + ∆𝐻𝑓𝑂2 ° ] Δ 𝐻𝑟 ° = [2(− 242)] − [0]⟹∆𝐻𝑟 ° = − 484 𝐾𝐽/𝑚𝑜𝑙 Δ 𝐺𝑟 ° = ∑ 𝑛 ∆𝐺𝑓(𝑃) ° ∑ 𝑛 ∆𝐺𝑓(𝑅) ° = ] 2Δ [ − ] 0 + 0 [ 𝐺𝑓𝐻2 𝑂 ° T = 25 + 273 T = 298 K Δ 𝐺𝑟 ° = [2(− 228)]⟹∆𝐺𝑟 ° = − 456 𝐾𝐽/𝑚𝑜𝑙 Δ 𝐺𝑟 ° = ∆𝐻𝑟 ° − 𝑇∆𝑆𝑟 ° - 456 = - 484 - ) 298 ( ∆𝑆𝑟 ° ⟹ ∆𝑆𝑟 ° = −28 298 = − 0. 094 𝐾𝐽/𝐾 𝑚𝑜𝑙 ∴ ∆𝑆𝑟 ° = − 0. 094 × 1000⟹ ∆𝑆𝑟 ° = − 94 𝐽/𝐾 𝑚𝑜𝑙 ‫اﻟﺳﺎدس‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬
  • 22. 1 . Δ𝐺𝑟 ° = Δ𝐻𝑟 ° − 𝑇∆𝑆𝑟 ° ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / T 2 . ) A ‫ﯾﺟب‬ ‫اﻟﺗﻣﯾﯾز‬ ‫ﺑﯾن‬ Δ ‫و‬ ‫وﺑﯾن‬ Δ ‫و‬ Δ . 𝐺𝑟 ° ∆𝐺°𝑓 𝐻𝑟 ° 𝐻𝑓 ° ) B ‫ﻗﯾم‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫واﻟطﺎﻗﺔ‬ ‫اﻟﺣرة‬ ‫ﻟﻠﻌﻧﺎﺻر‬ ‫اﻟﺣرة‬ ‫ﺑﺄﺛﺑت‬ ‫ﺻورة‬ ‫ﺗﺳﺎوي‬ 1 ) C ‫ﻗﯾم‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫واﻟطﺎﻗﺔ‬ ‫اﻟﺣرة‬ ‫ﻟﻠﻌﻧﺎﺻر‬ ‫اﻟﺣرة‬ ‫ﺑﺄﺛﺑت‬ ‫ﺻورة‬ ‫ﺗﺳﺎوي‬ ‫ﺻﻔر‬ (‫)ﺧﯾﺎرات‬ ‫اﻟﺳؤال‬ ‫ﻧوع‬ ‫اﻟﺟواب‬ / A& C 3 . ‫اﻟطﺎﻗﺔ‬ ‫ﻋﻠﻰ‬ ‫ﺗﻌﺗﻣد‬ ‫ﻻ‬ ‫ﻟﻠﺟزﯾﺋﺎت‬ (‫)اﻻﻧﺗروﺑﻲ‬ ‫اﻟﻌﺷواﺋﯾﺔ‬ ‫ﺻﻐﯾرة‬ ‫ﺣرﻛﺎت‬ ‫وھﻲ‬ ،‫اﻟﺣرﻛﯾﺔ‬ ‫اﻟﺣرة‬ ‫واﻟطﺎﻗﺔ‬ ‫اﻻﻧﺛﺎﻟﺑﻲ‬ ‫ﻟﻘﯾم‬ ‫ﺑﺎﻟﻧﺳﺑﺔ‬ ‫ﻟذﻟك‬ ‫ﺗﻛون‬ ‫وﺣدة‬ ΔS ‫ﺻﻐﯾرة‬ ‫ﺑﺎﻟﺟول‬ ) J ( ‫ووﺣدات‬ ΔH ‫و‬ ΔG ‫ﻛﺑﯾرة‬ ‫ﺑﺎﻟـ‬ ) KJ .( ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / F ( ‫اﻟﺳﺎﺑﻊ‬ ‫)اﻟدرس‬ ‫اﻟﺣرة‬ ‫ﻛﺑس‬ ‫طﺎﻗﺔ‬ ‫ﺗطﺑﯾﻘﺎت‬
  • 23. ‫س‬ 6 / ‫ﺟﺪ‬ ‫درﺟﺔ‬ ‫اﻟﺤﺮارة‬ ‫اﻟﺘﻲ‬ ‫ﺗﺼﺒﺢ‬ ‫ﻋﻨﺪھﺎ‬ ‫اﻟﺘﻔﺎﻋﻼت‬ ‫اﻟﺘﺎﻟﯿﺔ‬ ،‫ﺗﻠﻘﺎﺋﯿﺔ‬ ‫إذا‬ :‫ﻋﻠﻤﺖ‬ ‫ﻓرع‬ ) A /( ∆𝐻𝑟 = (+ 126) 𝐾𝐽/𝑚𝑜𝑙 ∆𝑆𝑟 = (+ 48) 𝐽/𝐾 𝑚𝑜𝑙 /‫اﻟﺣل‬ ΔG ‫ﻧﻔﺘﺮض‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻓﻲ‬ ‫ﺣﺎﻟﺔ‬ ،‫اﺗﺰان‬ ، ‫ﺻﻔﺮ‬ = ∴ ‫وﻧﻮﺣﺪ‬ ‫اﻟﻮﺣﺪات‬ ∆𝐻 ∆𝑆 = 𝑇⟹ 0 = ∆𝐻 − ∆𝑆 ∆𝑆𝑟 = 48 1000 ⟹ ∆𝑆𝑟 = + 0. 048 𝐾𝐽/𝐾 𝑚𝑜𝑙 ∴ 𝑇 = 126 0.048 ⟹ 𝑇 = 2625 𝐾 /‫ﻣﻼﺣظﺔ‬ ‫إذا‬ ‫ﻛﺎﻧﺖ‬ ‫إﺷﺎرة‬ ΔS ‫و‬ ΔH = ‫ﻣﻮﺟﺒﺔ‬ ‫ﻓﯿﺠﺐ‬ ‫ﺗﺴﺨﯿﻦ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻷﻛﺜﺮ‬ ‫ﻣﻦ‬ ‫درﺟﺔ‬ ‫اﻟﺤﺮارة‬ ‫اﻟﻤﺤﺴﻮﺑﺔ‬ ‫ﻋﻨﺪ‬ ‫اﻻﺗﺰان‬ . ‫وﻋﻠﯿﮫ‬ ‫ﯾﺠﺐ‬ ‫ﺗﺴﺨﯿﻦ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻷﻛﺜﺮ‬ ‫ﻣﻦ‬ ) 2625 K ( ‫ﻟﻜﻲ‬ ‫ﯾﺼﺒﺢ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ .‫ﺗﻠﻘﺎﺋﻲ‬ (B) ‫ﻓرع‬/ ∆𝑆𝑟 = (− 105) 𝐽/𝐾 𝑚𝑜𝑙, ∆𝐻𝑟 = (− 12) 𝐾𝐽/𝑚𝑜𝑙 ‫ﻧﻔﺘﺮض‬ ΔG = ‫ﺻﻔﺮ‬ ‫)ﺣﺎﻟﺔ‬ (‫اﻻﺗﺰان‬ ∴ 𝑇 = ∆𝐻 ∆𝑆 , ∆𝑆 = −105 1000 ⟹ ∆𝑆 = − 0. 105 𝐾𝐽/𝐾 𝑚𝑜𝑙 𝑇 = −12 −0.105 ⟹ 𝑇 = 114. 3 𝐾 ‫وﻋﻠﯿﮫ‬ ‫ﯾﺠﺐ‬ ‫ﺗﺒﺮﯾﺪ‬ ‫إﻧﺎء‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻷﻗﻞ‬ ‫ﻣﻦ‬ ) 114.3 K ( ‫ﻟﯿﺼﺒﺢ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ .‫ﺗﻠﻘﺎﺋﻲ‬ ‫داﺋﻤﺎ‬ ‫ﻓﻲ‬ ‫اﻟﺴﺆال‬ ‫ﻣﺘﺸﺎﺑﮭﺔ‬ ΔS ‫و‬ ΔH ‫ﺳﺘﻌﻄﻰ‬ ‫أﺷﺎرات‬ ‫ﻗﯿﻢ‬ ‫ﻣﻼﺣظﺔ‬/ = ‫ﺳﺎﻟﺒﺔ‬ ‫)ﻧﺒﺮداﻟﺘﻔﺎﻋﻞ‬ ) ΔS ‫و‬ ΔH ‫اذا‬ ‫ﻛﺎﻧﺖ‬
  • 24. ‫س‬ 7 : ‫ﺗﺘﻔﻜﻚ‬ ‫ﻛﺎرﺑﻮﻧﺎت‬ ‫اﻟﻜﺎﻟﺴﯿﻮم‬ ‫ﺣﺴﺐ‬ ‫اﻟﻤﻌﺎدﻟﺔ‬ ‫اﻵﺗﯿﺔ‬ : 𝐶𝑎𝐶𝑂3 (𝑠) ∆→ 𝐶𝑎𝑂(𝑠) + 𝐶𝑂2 (𝑔) (160 J/K mol) =Δ𝑆°𝑟 ‫ﻓﺈذا‬ ‫ﻋﻠﻤﺖ‬ Δ ‫ﻟﻜﻞ‬ ‫ﻣﻦ‬ ‫و‬ CaO ‫و‬ ‫ھﻲ‬ ‫ﻋﻠﻰ‬ :‫اﻟﺘﻮاﻟﻲ‬ 𝐻𝑓 ° 𝐶𝑂2 𝐶𝑎𝐶𝑂3 -) 1207 / - 635 / - 393.5 ( ‫ﺑﻮﺣﺪات‬ KJ/mol ، :‫ﺟﺪ‬ ‫ﻟﻠﺘﻔﺎﻋﻞ‬ ‫ﺛﻢ‬ ‫أرﺳﻢ‬ ‫ﻣﺨﻄﻂ‬ ‫اﻟﻄﺎﻗﺔ‬ Δ 1) 𝐻𝑟 ° ‫ﻟﻠﺘﻔﺎﻋﻞ‬Δ 2) 𝐺𝑟 ° 3) ‫درﺟﺔ‬ ‫اﻟﺤﺮارة‬ ‫اﻟﺘﻲ‬ ‫ﯾﺼﺒﺢ‬ ‫ﻋﻨﺪھﺎ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﺗﻠﻘﺎﺋﯿﺎ‬ /‫اﻟﺣل‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻣﺎص‬ 1 ( ∆𝐻𝑟 ° = ∑ 𝑛∆ 𝐻𝑓(𝑃) ° − ∑ 𝑛 ∆𝐻𝑓 𝑅 ( ) ° ∆𝐻𝑟 ° = [(− 635) + (− 393. 5)] − [− 1207] ∆𝐻𝑟 ° = (− 1028) + (1207) ∆𝐻𝑟 ° = 178. 5 𝐾𝐽/𝑚𝑜𝑙 ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻏﯿﺮ‬ ‫ﺗﻠﻘﺎﺋﻲ‬ 2 ( T = 25 + 273 = 298 K
  • 25. ∆𝑆𝑟 ° = 160 1000 = 0. 16 𝐾𝐽/𝐾 𝑚𝑜𝑙 ∴ ∆𝐺𝑟 ° = ∆𝐻𝑟 ° − 𝑇∆𝑆𝑟 ° ∆𝐺𝑟 ° = 178. 5 − (298) (0. 16) ∆𝐺𝑟 ° = 130. 82 𝐾𝐽/𝑚𝑜𝑙 3) (0 = Δ ‫ﻧﻔﺘﺮض‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫ﻣﺘﺰن‬ 𝐺𝑟 ° ) 0 = ∆𝐻𝑟 ° − 𝑇∆𝑆⟹𝑇 = ∆𝐻𝑟 ° ∆𝑆𝑟 ° ⟹ 𝑇 = 178.5 0.16 = 115. 6 𝐾 ‫ﻣﻮﺟﺒﺔ‬Δ ‫و‬ ‫ﺑﻤﺎ‬ ‫اﻧﮫ‬ ‫ﻗﯿﻤﺘﻲ‬ 𝐻𝑟 ° ∆𝑆𝑟 ° ‫ﻟﻜﻲ‬ ‫ﯾﺼﺒﺢ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ .ً‫ﺎ‬‫ﺗﻠﻘﺎﺋﯿ‬ 1115.6 K ً‫ا‬‫إذ‬ ‫ﯾﺠﺐ‬ ‫ﺗﺴﺨﯿﻦ‬ ‫اﻟﺘﻔﺎﻋﻞ‬ ‫إﻟﻰ‬ ‫أﻛﺜﺮ‬ ‫ﻣﻦ‬
  • 26. ‫اﻟﺳﺎﺑﻊ‬ ‫اﻟدرس‬ ‫اﺳﺋﻠﺔ‬ 1 . ‫إذا‬ ‫ﻛﺎﻧت‬ ‫إﺷﺎرة‬ ΔS ‫و‬ ΔH = ‫ﺳﺎﻟﺑﺔ‬ ‫ﻓﯾﺟب‬ ‫ﺗﺳﺧﯾن‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻷﻛﺛر‬ ‫ﻣن‬ ‫درﺟﺔ‬ ‫اﻟﺣرارة‬ .‫اﻻﺗزان‬ ‫ﻋﻧد‬ ‫اﻟﻣﺣﺳوﺑﺔ‬ ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / F 2 . ‫اذا‬ ‫ﻛﺎﻧت‬ S Δ ‫و‬ ΔH = ‫ﺳﺎﻟﺑﺔ‬ (‫)ﻧﺑرداﻟﺗﻔﺎﻋل‬ ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / F 3 . ‫ﯾﺟب‬ ‫ﺗﺳﺧﯾن‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻷﻛﺛر‬ ‫ﻣن‬ ) 2625 K ( ‫ﻟﻛﻲ‬ ‫ﯾﺻﺑﺢ‬ ‫اﻟﺗﻔﺎﻋل‬ .‫ﺗﻠﻘﺎﺋﻲ‬ ‫ﻧوع‬ ‫اﻟﺳؤال‬ ) T, F ( ‫اﻟﺟواب‬ / T