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‫اﻟﺸﻌﺒﻴﺔ‬ ‫اﻃﻴﺔ‬‫ﺮ‬‫اﻟﺪﻳﻤﻘ‬ ‫ﻳﺔ‬‫ﺮ‬‫اﺋ‬‫ﺰ‬‫اﻟﺠ‬ ‫ﻳﺔ‬‫ر‬‫اﻟﺠﻤﻬﻮ‬
‫ﻣﺴﺘﻐﺎﻧﻢ‬ ‫ﻟﻮﻻﻳﺔ‬ ‫ﺑﻴﺔ‬‫ﺮ‬‫اﻟﺘ‬ ‫ﻳﺔ‬‫ﺮ‬‫ﻣﺪﻳ‬
‫ﻋﺸﻌﺎﺷﺔ‬ ‫ﺛﺎﻧﻮﻳﺔ‬
)
‫اﻟﻘﺎدر‬ ‫ﻋﺒﺪ‬ ‫ﻳﻒ‬‫ﺮ‬‫ﺷ‬ ‫ﲪﺪي‬
(
‫اﻷول‬ ‫اﻟﻔﺼﻞ‬ ‫اﻣﺘﺤﺎن‬
‫اﺳﻴﺔ‬‫ر‬‫اﻟﺪ‬ ‫اﻟﺴﻨﺔ‬
:
2016
/
2017
‫اﻟﺸﻌﺒﺔ‬
:
‫ﻳﺎﺿﻴﺎت‬‫ر‬
‫اﻟﻤﺴﺘﻮى‬
:
‫اﻟﺜﺎﻟﺜﺔ‬ ‫اﻟﺴﻨﺔ‬
‫ﻣﺎدة‬ ‫ﻓﻲ‬ ‫اﺧﺘﺒﺎر‬
:
‫ﻳﺎﺋﻴﺔ‬‫ﺰ‬‫اﻟﻔﻴ‬ ‫اﻟﻌﻠﻮم‬
‫اﻟﻤﺪة‬
:
03
‫ﺳﺎﻋﺎت‬
‫أﺳﻮد‬ ‫أو‬ ‫أزرق‬ ‫ﺑﻘﻠﻢ‬ ‫إﺟﺎﺑﺘﻪ‬ ‫ﻳﺮ‬‫ﺮ‬‫ﺗﺤ‬ ، ‫اﻟﺘﻠﻤﻴﺬ‬ ‫ﻋﻠﻰ‬ : ‫ﻣﻼﺣﻈﺔ‬
‫اﻷول‬ ‫اﻟﺗﻣرﯾن‬
:
)
,0
5
0
‫ﻧﻘطﺔ‬
(
‫اﻟﻧظﯾر‬ ‫ﯾﻌﺗﺑر‬
	
‫ﺑﯾن‬ ‫ﻣن‬ ‫ﻟﻠﺗﻛﻧﺳﯾوم‬
‫اﻟﻣﺷﻌﺔ‬ ‫اﻷﻧوﯾﺔ‬
ّ‫ﺑ‬‫اﻟط‬ ‫اﻟﻣﺟﺎل‬ ‫ﻓﻲ‬ ‫اﻟﻣﺳﺗﻌﻣﻠﺔ‬
‫ﺧطورﺗﮫ‬ ‫وﻗﻠﺔ‬ ، ‫اﻟﻘﺻﯾرة‬ ‫ﺣﯾﺎﺗﮫ‬ ‫ﻟﻣدة‬ ‫اﻋﺗﺑﺎرا‬ ‫ﻲ‬
‫اﻷطﺑﺎء‬ ‫إﺷﺎرة‬ ‫رھن‬ ‫وﺿﻌﮫ‬ ‫وﺳﮭوﻟﺔ‬ ‫اﻟﻣﻧﺧﻔﺿﺔ‬ ‫وﺗﻛﻠﻔﺗﮫ‬ ‫اﻹﺷﻌﺎﻋﯾﺔ‬
.
1
(
‫ﯾﻌﺗﺑر‬
	
‫و‬
‫ﻟﻠﺗﻛﻧﯾﺳﯾوم‬ ‫ﻧظﯾران‬
.
1
-
1
(
‫و‬ ‫اﻟﻣﺷﻌﺔ‬ ‫اﻟﻧواة‬ ‫ف‬ّ‫ﻋر‬
‫اﻟﻧظﯾر‬ ‫ﻧواة‬ ‫ﺗرﻛﯾب‬ ‫اﻋط‬
.
1
-
2
(
‫اﺳﺗﻘرارا‬ ‫اﻷﻛﺛر‬ ‫اﻟﻧواة‬ ‫اﻟﺗﻌﻠﯾل‬ ‫ﻣﻊ‬ ‫ّد‬‫د‬‫ﺣ‬
.
1
-
3
(
‫اﻟﺗﻛﻧﺳﯾوم‬ ‫ﯾﻧﺗﺞ‬
‫اﻟﻣوﻟﯾﺑدان‬ ‫ﻧواة‬ ‫ﺗﻔﻛك‬ ‫ﻋن‬
( è )
.
‫أ‬
-
‫اﻟﺗﻛﻧﺗﯾوم‬ ‫ﻹﻧﺗﺎج‬ ‫اﻟﻧووي‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫أﻛﺗب‬
	
‫اﻟﻣوﻟﯾﺑدان‬ ‫ﻣن‬ ‫اﻧطﻼﻗﺎ‬
.
‫؟‬ ‫اﻟﺣﺎﺻل‬ ‫اﻟﺗﻔﻛك‬ ‫ﻧﻣط‬ ‫ﻣﺎھو‬
‫ب‬
-
‫اﻟﻣﺗﺣررة‬ ‫اﻟطﺎﻗﺔ‬ ‫أﺣﺳب‬ ‫اﻟﺣﺎدث‬ ‫اﻟﻧووي‬ ‫اﻟﺗﺣول‬ ‫ﯾواﻓق‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫ﻣﺧططﺎ‬ ‫أﻧﺟز‬
ℓ
‫ذﻟك‬ ‫ﺧﻼل‬
.
2
(
‫اﻟﺗﻛﻧﺳﯾوم‬ ‫ﯾﺳﺗﻌﻣل‬
‫ﺑﺟرﻋﺔ‬ ‫اﻹﻧﺳﺎن‬ ‫ﺟﺳم‬ ‫ﺣﻘن‬ ‫ﯾﺗم‬ ‫ﺣﯾث‬ ، ‫ﺗﺷﺧﯾﺻﮭﺎ‬ ‫ﻗﺻد‬ ‫اﻹﻧﺳﺎن‬ ‫ﻟﻌظﺎم‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫ﺑﺎﻟﻧﺷﺎط‬ ‫اﻟﺗﺻوﯾر‬ ‫ﻓﻲ‬
‫اﻟﻣﺷﻊ‬ ‫اﻟﺗﻛﻧﯾﺗﯾوم‬ ‫ﻋﻠﻰ‬ ‫ﺗﺣﺗوي‬
‫اﻟﻣﻔﺣوﺻﺔ‬ ‫ﻟﻠﻌظﺎم‬ ‫ﺻورة‬ ‫ﻋﻠﻰ‬ ‫ﻟﻠﺣﺻول‬ ‫زﻣﻧﯾﺔ‬ ‫ﻣدة‬ ‫ﺑﻌد‬ ‫ُﺳﺗﻛﺷف‬‫ﯾ‬ ‫واﻟذي‬
.
‫ﻓﻲ‬ ‫ﻧﻌطﻲ‬
‫اﻟﺷﻛل‬
-
1
-
‫اﻷ‬ ‫ﻋدد‬ ‫ﺑدﻻﻟﺔ‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﻟﺗﻐﯾرات‬ ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬
‫اﻟﻣﺗﻔﻛﻛﺔ‬ ‫ﻧوﯾﺔ‬
= ( )
.
2
-
1
(
‫أ‬
-
‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫أوﺟد‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬
	
‫ﻟﻠﺗﻛﻧﯾﺳﯾوم‬
.
‫ب‬
-
‫ھﻲ‬ ‫ﻟﮫ‬ ‫اﻟﻌﻣر‬ ‫ﻧﺻف‬ ‫زﻣن‬ ‫ﻗﯾﻣﺔ‬ ّ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬
:
½ =
.
‫ﻋﻧد‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫ﻧﺷﺎطﮭﺎ‬ ‫ﺑﺣﻘﻧﺔ‬ ‫إﻧﺳﺎن‬ ‫ﺟﺳم‬ ‫ﺣﻘن‬ ‫ﺗم‬
= 0
‫ھو‬
‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ‫اﻟﻣﻔﺣوﺻﺔ‬ ‫ﻟﻠﻌظﺎم‬ ‫ﺻورة‬ ‫أﺧذ‬ ‫ﻟﯾﺗم‬
‫ﺗﺻﺑﺢ‬ ‫ﺣﯾث‬
‫ﻋﻧدھﺎ‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﻗﯾﻣﺔ‬
t 	
‫ھو‬
60%
‫ﻗﯾﻣﺔ‬ ‫ﻣن‬
.
2
-
2
(
‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬
‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬ ‫ﺑﮭﺎ‬ ‫اﻟﺟﺳم‬ ‫ﺣﻘن‬ ‫ﺗم‬ ‫اﻟﺗﻲ‬ ‫اﻟﻣﺷﻌﺔ‬ ‫اﻷﻧوﯾﺔ‬ ‫ﻋدد‬
= 0
.
2
-
3
-
(
‫ﺑﺎﻟﺳﺎﻋﺔ‬ ‫ﺣدد‬
)
ℎ
(
‫ﻗﯾﻣﺔ‬
.
‫اﻟﻣﻌطﯾﺎت‬
:
1	 	 = 	931,5	 .
،
= 1,0073	
= 0,00055	
،
= 1,0087	
‫اﻟﺼﻔﺤﺔ‬
1
/
4
‫اﻟﻧواة‬
( )
( )
( 	)
ℓ( )
ℓ =
852,10	
ℓ =
852,53	
ℓ =
836,28
‫اﻟﺗﻣرﯾن‬
‫اﻟﺛﺎﻧﻲ‬
:
)
,0
6
0
‫ﻧﻘطﺔ‬
(
‫ﻧﺿﻊ‬
‫ﻛﺄس‬ ‫ﻓﻲ‬
‫ﺣﺟﻣﺎ‬
‫اﻟﺻودﯾوم‬ ‫ﻟﮭﯾدروﻛﺳﯾد‬ ‫ﻣﺎﺋﻲ‬ ‫ﻣﺣﻠول‬ ‫ﻣن‬
)
( )	, ( )
(
‫ﻣﺎدﺗﮫ‬ ‫ﻛﻣﯾﺔ‬
‫اﻟﻣوﻟﻲ‬ ‫وﺗرﻛﯾزه‬
= 10	 ℓ.
‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ‫إﻟﯾﮫ‬ ‫ﻧﺿﯾف‬ ‫ﺛم‬
= 0
‫اﻟﻣﺎدة‬ ‫ﻛﻣﯾﺔ‬ ‫ﻧﻔس‬ ،
‫ﺗﻔﺎﻋﻠﻲ‬ ‫ﺧﻠﯾط‬ ‫ﻋﻠﻰ‬ ‫ﻟﻧﺣﺻل‬ ‫اﻹﯾﺛﯾل‬ ‫إﯾﺗﺎﻧوات‬ ‫ﻣن‬
‫ﺣﺟﻣﮫ‬ ‫اﻟﻣوﻻت‬ ‫ﻣﺗﺳﺎوي‬
≈ = 10
.
‫ﻧﻧﻣذج‬
‫ﺑﯾن‬ ‫ﯾﺣدث‬ ‫اﻟذي‬ ‫اﻟﻛﯾﻣﯾﺎﺋﻲ‬ ‫اﻟﺗﺣول‬
‫اﻹﯾﺛﯾل‬ ‫إﯾﺗﺎﻧوات‬
‫و‬
‫اﻟﺻودﯾوم‬ ‫ﻟﮭﯾدروﻛﺳﯾد‬
‫اﻟﺗﺎﻟﯾﺔ‬ ‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬
:
	 (ℓ) + ( )	−→ ( ) + − ( )
1
-
‫أ‬
-
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬ ‫واﺳﺗﻧﺗﺞ‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻟﺗﻘدم‬ ‫ﺟدوﻻ‬ ‫أﻧﺟز‬
.
‫ب‬
-
‫اﻟﺗﻔ‬ ‫ﻟﻠوﺳط‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻋﺑﺎرة‬ ‫أﻛﺗب‬
‫ﺎﻋﻠﻲ‬
:

)
‫ﻋﻧد‬
= 0
(
.

( )
)
‫ﻟﻣﺎ‬
> 0
(
‫ﺑدﻻﻟﺔ‬
،
،
	
،

‫و‬

.
‫ج‬
-
‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬
= ( )
‫ا‬
‫ﻟﺷﻛل‬
)
2
(
‫ﻋﺑﺎرة‬ ‫أﻛﺗب‬
( )
‫ﺑدﻻﻟﺔ‬
.
‫د‬
-
‫اﻟﺳؤاﻟﯾن‬ ‫ﺑﺈﺟﺎﺑﺔ‬ ‫ﺑﺎﻻﺳﺗﻌﺎﻧﺔ‬
)
‫ب‬
–
‫ج‬
(
‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﺗﻧﺎﻗص‬ ‫ﺳﺑب‬ ‫ّن‬‫ﯾ‬‫ﺑ‬
‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫اﻟوﺳط‬ ‫ﻓﻲ‬ ‫اﻟﻧوﻋﯾﺔ‬
.
2
-
‫اﻟﻛﯾﻣﺎﺋﻲ‬ ‫اﻟﺗﺣول‬ ‫ﻟﺗطور‬ ‫اﻟزﻣﻧﯾﺔ‬ ‫اﻟﻣﺗﺎﺑﻌﺔ‬
:
‫ﺗطور‬ ‫ﻧﺗﺗﺑﻊ‬
‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻗﯾﺎس‬ ‫طرﯾق‬ ‫ﻋن‬ ‫اﻟﻛﯾﻣﺎﺋﻲ‬ ‫اﻟﺗﺣول‬
‫ﺑواﺳطﺔ‬ ‫ﻟﻧﺣﺻل‬ ‫اﻟزﻣن‬ ‫ﺧﻼل‬ ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠﻣزﯾﺞ‬ ‫اﻟﻧوﻋﯾﺔ‬
‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﻣﻌﻠوﻣﺎﺗﯾﺔ‬ ‫ﺑرﻣﺟﯾﺔ‬
= ( )
‫اﻟﺷﻛل‬ ‫ﻓﻲ‬
)
3
(
.
2
-
1
(
‫أﺣﺳب‬
½
‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬
‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠﺧﻠﯾط‬
‫ﺛم‬
‫اﻟﺗﻔﺎﻋل‬ ‫ﻧﺻف‬ ‫زﻣن‬ ‫اﺳﺗﻧﺗﺞ‬
½
.
2
-
3
(
‫اﻟﺗﻔﺎﻋل‬ ‫ﺣرﻛﯾﺔ‬
:
‫أ‬
(
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﻋرف‬
‫ﺑدﻻﻟﺔ‬ ‫ﻋﺑﺎرﺗﮭﺎ‬ ‫أوﺟد‬ ‫ﺛم‬
( )
.
‫ب‬
-
‫ﺑﺎﻟوﺣدة‬ ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫أﺣﺳب‬
)
ℓ	. .
(
‫اﻟﻠﺣظﺗﯾن‬ ‫ﻋﻧد‬
) :
= 0
(
‫و‬
)
= 35
(
.
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﺗطور‬ ‫اﺷرح‬
.
‫ﻣﻌطﯾﺎت‬
:
‫اﻟﺷﺎردة‬
( )
( )
( )
‫ﺑـ‬ ‫اﻟﺷﺎردﯾﺔ‬ ‫اﻟﻣوﻟﯾﺔ‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬
‫ى‬
)
. .
(



‫اﻟﺼﻔﺤﺔ‬
2
/
4
‫اﻟﺗﻣرﯾن‬
‫اﻟﺛﺎﻟث‬
:
)
5
04,
‫ﻧﻘطﺔ‬
(
‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟدارة‬ ‫ﺗﻌﺗﺑر‬
‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻷﺟﮭزة‬ ‫ﻣن‬ ‫ﻟﻣﺟﻣوﻋﺔ‬ ‫اﻹﻟﻛﺗروﻧﯾﺔ‬ ‫اﻟﺗراﻛﯾب‬ ‫ﻓﻲ‬ ‫اﻟﻣﺳﺗﻌﻣﻠﺔ‬ ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟدارات‬ ‫ﺑﯾن‬ ‫ﻣن‬
.
‫ﻓﻲ‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺗرﻛﯾب‬ ‫ﯾﺗﻛون‬
‫اﻟﺷﻛل‬
-
4
-
‫ﻣن‬
:
-
‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟﻣﺣرﻛﺔ‬ ‫ﻗوﺗﮫ‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﺛﺎﻟﻲ‬ ‫ﻣوﻟد‬
.
-
‫ﺳﻌﺗﺎھﻣﺎ‬ ‫ﻣﻛﺛﻔﺗﯾن‬
	
‫و‬
= 2
.
-
‫ﻣﻘﺎوﻣﺗﮫ‬ ‫اوﻣﻲ‬ ‫ﻧﺎﻗل‬
= 3 
.
-
‫ﻟﻠﺗﯾﺎر‬ ‫ﻗﺎطﻌﺔ‬
	
.
‫ﻟﻸزﻣﻧﺔ‬ ‫ﻣﺑدءا‬ ‫ﻧﺧﺗﺎرھﺎ‬ ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬
)
= 0
(
‫اﻟﻘﺎطﻌﺔ‬ ‫ﻧﻐﻠق‬ ،
.
1
-
‫اﻟﺳﻌﺔ‬ ‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬
Cé
‫ھﻲ‬ ‫اﻟدارة‬ ‫ﻓﻲ‬ ‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫ﻟﻠﻣﻛﺛﻔﺔ‬
:
1. 2
1+ 2
Cé =
.
2
-
‫أ‬
-
‫اﻟﺗوﺗر‬ ‫ﯾﺣﻘﻘﮭﺎ‬ ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬
( )
‫ذ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫طرﻓﻲ‬ ‫ﺑﯾن‬
‫ات‬
‫اﻟﺳﻌﺔ‬
‫ﺗﻛﺗب‬
‫ﺑﺎﻟﺷﻛل‬
:
( )
+
	 é
2( ) =
	 2
‫ب‬
-
‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ھذه‬ ‫ﺣل‬ ‫ﯾﻛﺗب‬
‫اﻟﺷﻛل‬ ‫ﻋﻠﻰ‬
:
( ) = (1 − ∝	
)
.
-
‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻣن‬ ‫ﻛل‬ ‫ﻋﺑﺎرة‬ ‫ﺣدد‬
‫و‬
∝
‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬
.
‫ج‬
-
‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫ﻋﺑﺎرة‬ ‫اوﺟد‬
( )
‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﺷﺣﻧﺔ‬ ‫وﻛذا‬
( )
.
3
-
‫ﯾﻣﺛل‬
②
‫و‬
①	
‫ﻣﻧﺣﻧﯾﺎ‬
‫اﻟﺷﻛل‬
–
5
-
‫اﻟﻛﮭرﺑﺎﺋﯾﯾن‬ ‫اﻟﺗوﺗرﯾن‬ ‫ﺗطور‬
( )
‫و‬
( )
.
‫أ‬
-
‫اﻟﺗﺑرﯾر‬ ‫ﻣﻊ‬ ‫اﻟﻣﻧﺎﺳب‬ ‫ﻟﻠﺗوﺗر‬ ‫ﺑﯾﺎﻧﻲ‬ ‫ﻣﻧﺣﻧﻰ‬ ‫ﻛل‬ ‫أﻧﺳب‬
.
‫ب‬
-
‫اﻟﺗوﺗر‬ ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬
‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫وأﺣﺳب‬
.
‫ج‬
-
‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫ﺑﯾﺎﻧﯾﺎ‬ ‫أوﺟد‬
‫ﺛم‬
‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬
:
= 4
.
4
-
‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫اﻷﻋظﻣﯾﺔ‬ ‫اﻟﻘﯾﻣﺔ‬ ‫أﺣﺳب‬
.
‫اﻟراﺑﻊ‬ ‫اﻟﺗﻣرﯾن‬
:
)
5
,
4
0
‫ﻧﻘطﺔ‬
(
‫ﻓﻲ‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺗرﻛﯾب‬ ‫ﻧﻧﺟز‬
‫اﻟﺷﻛل‬
-
6
-
‫ﻣن‬ ‫واﻟﻣﻛون‬
:
-
‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟﻣﺣرﻛﺔ‬ ‫ﻗوﺗﮫ‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﺛﺎﻟﻲ‬ ‫ﻣوﻟد‬
= 12
-
‫وﺷﯾﻌﺔ‬
‫ﻣﺛﺎﻟﯾﺔ‬
‫ﺗﺣرﯾﺿﮭﺎ‬ ‫ﻣﻌﺎﻣل‬
)
‫ذاﺗﯾﺗﮭﺎ‬
(
.
-
‫اوﻣﯾﯾن‬ ‫ﻧﺎﻗﻠﯾن‬
‫ﻣﻘﺎوﻣﺎﺗﮭﻣﺎ‬
= 40
‫و‬
-
‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫ﻟﻠﺗﯾﺎر‬ ‫ﻗﺎطﻌﺔ‬
.
‫اﻟﺼﻔﺤﺔ‬
3
/
4
‫ﻟﻸزﻣﻧﺔ‬ ‫ﻣﺑدءا‬ ‫ﻧﺧﺗﺎرھﺎ‬ ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬
)
= 0
(
‫اﻟﻘﺎطﻌﺔ‬ ‫ﻧﻐﻠق‬ ،
‫ﺑﺎﻟدارة‬ ‫ﻣوﺻل‬ ‫ﻣﻌﻠوﻣﺎﺗﻲ‬ ‫ﻧظﺎم‬ ‫وﺑواﺳطﺔ‬
)
‫ﯾظﮭر‬ ‫ﻻ‬
‫اﻟدارة‬ ‫ﻓﻲ‬
(
‫اﻟﻣﻧﺣﻧﯾﯾن‬ ‫ﻋﻠﻰ‬ ‫ﻧﺣﺻل‬
( )
‫و‬
( )
‫اﻟﻣدﺧﻠﯾن‬ ‫ﻋﻧد‬ ‫ﻟﻠﺗوﺗرﯾن‬ ‫اﻟﻣﻣﺛﻠﯾن‬
A
‫و‬
B
‫اﻟﺷﻛل‬
-
7
-
.
1
-
‫اﻟﺗوﺗر‬ ‫ﯾﻣﺛل‬ ‫اﻟذي‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ّن‬‫ﯾ‬‫ﻋ‬
( )
‫اﻟﺗوﺗر‬ ‫ﯾﻣﺛل‬ ‫اﻟذي‬ ‫واﻟﻣﻧﺣﻧﻰ‬
( )
.
2
-
‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬
‫اﻟداﺋم‬ ‫اﻟﻧظﺎم‬ ‫ﻓﻲ‬ ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ،
.
3
-
‫اﻟﻣﻘﺎوﻣﺔ‬ ‫ﻗﯾﻣﺔ‬ ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬
‫ﻟﻠﻧﺎﻗل‬
‫اﻷوﻣﻲ‬
‫ھﻲ‬
= 8	
.
4
-
‫أﺛﺑت‬ ‫اﻟﺗوﺗرات‬ ‫ﺟﻣﻊ‬ ‫ﻗﺎﻧون‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬
‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬
‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗوﺗر‬ ‫ﯾﺣﻘﻘﮭﺎ‬
( )
.
5
-
‫اﻟﺷﻛل‬ ‫ﻣن‬ ‫ھو‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﺣل‬ ‫أن‬ ‫ﻋﻠﻣﺎ‬
:
(1 − )
( )	=
.
‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻋﺑﺎرﺗﻲ‬ ‫أوﺟد‬
‫و‬
‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬
.
6
-
‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬
‫ﻟﻠدارة‬
.
7
-
‫اﻟﺗﺣرﯾض‬ ‫ﻣﻌﺎﻣل‬ ‫ﻗﯾﻣﺔ‬ ‫اﺳﺗﻧﺗﺞ‬
‫ﻟﻠوﺷﯾﻌﺔ‬
.
8
-
‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬ ‫اﻟوﺷﯾﻌﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫اﻟطﺎﻗﺔ‬ ‫أﺣﺳب‬
=
.
‫اﻟﺼﻔﺤﺔ‬
4
/
4
‫ﻋﺒﺪاﻟﻘﺎدر‬ ‫ﻳﻒ‬‫ﺮ‬‫ﺷ‬ ‫ﺣﻤﺪي‬ ‫ﺛﺎﻧﻮﻳﺔ‬
–
‫ﻋﺸﻌﺎﺷﺔ‬
-
‫ﻟﻤﺎدة‬ ‫اﻷول‬ ‫اﻟﻔﺼﻞ‬ ‫اﻣﺘﺤﺎن‬ ‫ﺗﺼﺤﻴﺢ‬
‫ﻳﺎﺋﻴﺔ‬‫ﺰ‬‫اﻟﻔﻴ‬ ‫اﻟﻌﻠﻮم‬
–
‫اﻟﺜﺎ‬ ‫اﻟﺴﻨﺔ‬
‫ﻟﺜﺔ‬
‫ﺷﻌﺒ‬
‫ﺔ‬
)
‫ﻳﺎﺿﻴﺎت‬‫ر‬
(
‫اﺳﻴﺔ‬‫ر‬‫اﻟﺪ‬ ‫اﻟﺴﻨﺔ‬
:
2016
-
2017
‫د‬
-
‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﺗﻧﺎﻗص‬ ‫ﺳﺑب‬
‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫اﻟوﺳط‬ ‫ﻓﻲ‬ ‫اﻟﻧوﻋﯾﺔ‬
.
‫اﻟﻌﻼﻗﺗﯾن‬ ‫ﺑﻣطﺎﺑﻘﺔ‬

‫و‬

:
 −  < 0	 ⇒  < 
2
-
1
(
‫ﺣﺳ‬
‫ﺎ‬
‫ب‬
½
‫اﺳﺗﻧﺗ‬ ‫ﺛم‬
‫ﺎ‬
‫ج‬
½
.
σ½
= 0,25 − 160	 2
⇒ σ½
= 0,17	 . −1
= 170	 . −1
⟹ ½ = 12	
2
-
1
-
‫اﻟﺗﻔﺎﻋل‬ ‫ﺣرﻛﯾﺔ‬
:
‫أ‬
(
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬
‫ﺑدﻻﻟﺔ‬ ‫ﻋﺑﺎرﺗﮭﺎ‬
( )
:
‫واﺣدة‬ ‫ﻓﻲ‬ ‫اﻟزﻣن‬ ‫ﺧﻼل‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﺗﻘدم‬ ‫ﺗﻐﯾرات‬ ‫ﻣﻘدار‬ ‫ھﻲ‬
‫وﻧﻛﺗب‬ ‫اﻟﺣﺟوم‬
:
=
= −
,
‫ب‬
-
‫ﺣﺳ‬
‫ﺎ‬
‫ب‬
‫ﺑﺎﻟوﺣدة‬
)
ℓ	. .
(
‫ﻋﻧد‬
‫اﻟﻠﺣظﺗﯾن‬
) :
= 0
(
‫و‬
)
= 35
. (
= ×
‖ ‖
‖ ‖
(0) = 0,52	 ℓ	. . 	
(35min) = 0,083 ℓ	. .
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﺗطور‬ ‫ﺷرح‬
.
(0) > (35min)
‫ﺧﻼل‬ ‫اﻟﻣﺗﻔﺎﻋﻼت‬ ‫ﺗراﻛﯾز‬ ‫ﺗﻧﺎﻗص‬ ‫ﺑﺑﺳﺑب‬ ‫ﺗﺗﻧﺎﻗص‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﺳرﻋﺔ‬
‫اﻟزﻣن‬
.
‫ﻧﺟد‬ ‫ﺑﺎﻟﻣطﺎﺑﻘﺔ‬
:
= . = = 5. 10 	
Bq	
 = − = ×
‖ ‖
‖ ‖
= 3,22. 10
‫ب‬
-
ّ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬
½ = 	
:
½ =
ℓ
		
= , . ≈ 	
2
-
2
-
‫ﻗﯾﻣﺔ‬
‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬
= 0
:
= . ⇒ = 
= 1,55. 10
2
-
3
-
‫ﺗ‬
‫ﺣد‬
‫ﯾ‬
‫ﺑﺎﻟﺳﺎﻋﺔ‬ ‫د‬
)
ℎ
(
‫ﻗﯾﻣﺔ‬
:
= 0. −	 ⇒ 0,60 = 
⇒ =

ℓ 0
= 4,4	ℎ
‫اﻟﺛﺎﻧﻲ‬ ‫اﻟﺗﻣرﯾن‬
06
‫ﻧﻘط‬
:
1
-
‫أ‬
-
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬ ‫واﺳﺗﻧﺗﺞ‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻟﺗﻘدم‬ ‫ﺟدوﻻ‬ ‫أﻧﺟز‬
.
‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬
:
− = 0 ⟹ = = = 10 ℓ
‫ب‬
-
‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠوﺳط‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻋﺑﺎرة‬
:
=  	[ ] +  [ ] ⟹ = ( 	 +  )
( ) =  	[ ] +  [ ] +  2 3 2( )
−
( ) =  	 + 
	
+  = ( 	 +  ) + ( −  )

………………
( ) = + ( −  )
‫ج‬
-
‫ﻋﺑﺎرة‬
( )
‫ﺑدﻻﻟﺔ‬
.
( ) = +
= = 0,25	 .
= ×
‖ ‖
‖ ‖
≈ −160	 /	 . ℓ.

…
…………………
⇒ ( ) = 0,25 − 160	
	 (ℓ) + ( )	−→ ( ) + − ( )
‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬
‫ﺑـ‬ ‫اﻟﻣﺎدة‬ ‫ﻛﻣﯾــــــــــﺎت‬
( ℓ)
‫اﻟﺗﻘدم‬
‫اﻟ‬
‫ﺣﺎﻟﺔ‬
0
0
‫إﺑﺗدا‬
−
−
‫اﻧﺗﻘﺎ‬
−
−
‫ﻧﮭﺎ‬
‫اﻷول‬ ‫اﻟﺗﻣرﯾن‬
:
06
‫ﻧﻘطﺔ‬
1
-
1
(
‫اﻟﻧظﯾر‬ ‫ﻧواة‬ ‫ﺗرﻛﯾب‬
:
43 + 56	
1
-
2
(
‫اﻟﺗﻌﻠﯾل‬ ‫ﻣﻊ‬ ‫اﺳﺗﻘرارا‬ ‫اﻷﻛﺛر‬ ‫اﻟﻧواة‬
.
ℓ 	
= 8,621 / é 	
ℓ
= 8,611 / é
‫اﻟﻧواة‬
	
‫اﻟﻧواة‬ ‫ﻣن‬ ‫اﺳﺗﻘرارا‬ ‫أﻛﺛر‬
‫ﻷن‬
⇒ ℓ 	
> ℓ
3
-
‫أ‬
-
‫اﻟﺗﻛﻧﺗﯾوم‬ ‫ﻹﻧﺗﺎج‬ ‫اﻟﻧووي‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬
	
.
	⟶ +	
‫ﺻودي‬ ‫ﻗﺎﻧوﻧﻲ‬ ‫ﺣﺳب‬
99 = 99 +
42 = 43 +
⇒
= 0
= −1
⟹	 ⇛
‫اﻟﺗﻔﻛك‬ ‫ﻧﻣط‬
:
)
‫اﻟﻛﺗرون‬
(
	⟶ +	
‫ب‬
-
‫وﺣﺳ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫ﻣﺧطط‬
‫ﺎ‬
‫اﻟﻣﺗﺣررة‬ ‫اﻟطﺎﻗﺔ‬ ‫ب‬
ℓ
:
ℓ = − ℓ + + − . − ℓ
ℓ = −[852,10	 + (1,0073 + 0,00055 − 1,0087).931,5 − 852,53]
= 737,96	
2
-
1
(
‫أ‬
-
‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬
= ( )
‫إﯾﺟﺎد‬
	
‫ﻟـ‬
.
‫ﻟدﯾﻧﺎ‬
:
( ) = 	 ( ) = . − . … … … … . ‫	ﻧظرﯾﺎ‬
( ) = + . … … … … … … … … . . … . ‫	ﺑﯾﺎﻧﯾﺎ‬
⇒ =
− ( )
⇒ =
12 − 10
0,25
= 8	
4
-
‫ﺗﺣﻘﻘﮭﺎ‬ ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬
( )
:
∀	 ≥ 0	 ∶ ( ) + ( ) + ( ) = 	
( ) =
( )
=
( )
⇒
( ) =
( )
( ) =
( )
⇒ ( ) +
( )
+
( )
=
⟹
( )
+
( )
( ) =
5
-
‫اﻟﺷﻛل‬ ‫ﻣن‬ ‫ھو‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﺣل‬
:
.
(1 − )
( )	=
-
‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻋﺑﺎرﺗﻲ‬ ‫إﯾﺟﺎد‬
:
‫و‬
( )
= A.
A. +
( )
−
( )
=
⇒
( + ) =
=
( ) ⇒
= ( )
=
=
( )
6
-
‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬
‫ﻟﻠدارة‬
:
‫اﻟﺑﯾﺎن‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬
(
‫ﻧﺣﺳب‬
:
( ) = 0,63 (max) = 6,3	 ⇒ =
7
-
‫اﻟﺗﺣرﯾض‬ ‫ﻣﻌﺎﻣل‬ ‫ﻗﯾﻣﺔ‬
‫ﻟﻠوﺷﯾﻌﺔ‬
:
=
( )
⇒ = 	 ( + ) ⇒ = 	
8
-
‫اﻟطﺎ‬ ‫أﺣﺳب‬
‫ﻋﻧد‬ ‫اﻟوﺷﯾﻌﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻗﺔ‬
:
=
( ) = 	½ ( ) ⇒ ( )⌋ = = 	½ ( )
= = 1,5 ⇒ = 4
⇒ = ,
( )⌋ = , . 	. ,
⇒ ( )⌋ = , 	
3
-
‫أ‬
-
‫اﺳ‬
‫ﻧﺎد‬
‫اﻟﺗﺑرﯾر‬ ‫ﻣﻊ‬ ‫اﻟﻣﻧﺎﺳب‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﻧﺣﻧﻰ‬ ‫ﻛل‬
.
(0) = 0	
( ) = 0
⇒
(0) =
( ) = 0
‫اﻟﻣﻧﺣﻧﻰ‬

‫ﻟﻠﺗوﺗر‬
( )
2(0) = 0	
2( ) = .
‫اﻟﻣﻧﺣﻧﻰ‬

‫ﻟﻠﺗوﺗر‬
( )
‫ب‬
-
‫اﻟﺗوﺗر‬ ‫ﻗﯾﻣﺔ‬
‫اﻷﻋظﻣﻲ‬ ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫وﺣﺳﺎب‬
:
= (0)
= =
.
=
⇒
= 12	
= 4. 10
‫ج‬
-
‫ﺗ‬
ّ‫ﯾ‬‫ﺑ‬
‫ﺎ‬
‫أن‬ ‫ن‬
:
=
:
‫ﺑﯾﺎﻧﯾﺎ‬ ‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻧﺣﺳب‬
:
‫اﻟﺑﯾﺎن‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬

⇒ 	 = 4	 	
( ) = 0,37 = 4,44	
= 	 é 	⇒ é = ⇒ é =
4
3
	 	
+ =
é
⇒ =
é
− = ⇒ C = 4	μ	F
4
-
‫ﺣﺳ‬
‫ﺎ‬
‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫اﻷﻋظﻣﯾﺔ‬ ‫اﻟﻘﯾﻣﺔ‬ ‫ب‬
:
( ) = 	½Cé
2
= ½
. 2
( ) =
3
8
. 144 = 54	 	
‫اﻟﺗﻣرﯾن‬
‫اﻟراﺑﻊ‬
:
)
0
0
.
4
‫ﻧﻘطﺔ‬
(
1
-
‫اﻟﻣﻧﺣﻧﯾﯾن‬ ‫اﺳﻧﺎد‬
:
∀	 ≥ 0	 ∶	
( ) = − 	 ( )
( ) = ( )
	
(0) = 		,			 ( ) = −
(0) = 0) = 0		, ( ) = 	
‫اﻟﻣﻧﺣﻧﻰ‬ ‫وﻣﻧﮫ‬
( )
‫ﯾواﻓق‬
( )
‫و‬
‫اﻟﻣﻧﺣﻧﻰ‬
( )
‫ﻟـ‬
( )
2
-
‫ﻗﯾﻣﺔ‬
:
( ) =
( ) = 10	
⇒ =
( )
= = 0,25	
3
-
‫اﻟﻣﻘﺎوﻣﺔ‬ ‫ﻗﯾﻣﺔ‬ ‫أن‬ ‫ﻣن‬ ‫اﻟﺗﺣﻘق‬
‫ھﻲ‬ ‫اﻷوﻣﻲ‬ ‫ﻟﻠﻧﺎﻗل‬
= 	
.
‫اﻟﺛﺎﻟث‬ ‫اﻟﺗﻣرﯾن‬
:
)
0
0
.
4
‫ﻧﻘطﺔ‬
(
=?	
‫و‬
= 2
.
=? = 3 
1
-
‫ﺗﺑﯾﺎن‬
‫أن‬
:
1. 2
1+ 2
Cé =
.
= =
+ = + =
é
⇒
1
C1
+
1
C2
=
1
é
⇒ Cé =		 1. 2
1+ 2
	
2
-
‫أ‬
-
‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬
( )
:
( )
+
	 é
2( ) =
	 2
∀	 ≥ 0 ∶ ( ) + ( ) + ( ) =
‫اﻟﺗوﺗرات‬ ‫ﺟﻣﻊ‬ ‫ﻗﺎﻧون‬
( ) = = =
( )
( ) =
é
−
⇒
( )
+
é
=

………….
⟹
( )
+
	 é
( ) =
	
‫ب‬
-
‫اﻟﺷﻛل‬ ‫ﻋﻠﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ھذه‬ ‫ﺣل‬
:
( ) = (1 − ∝	
)
.
‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻣن‬ ‫ﻛل‬ ‫ﻋﺑﺎرة‬
‫و‬
∝
‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬
2
= A ∝ −∝	
‫ﻓﻲ‬ ‫ﺑﺎﻟﺗﻌوﯾض‬

:
⇒ A ∝ ∝	
+
	 é
−
	 é
A ∝	
=
	
	
⇒ A ∝	
∝ −
	 é
=
	
−
	 é
∝ −
1
	 é
= 0
	 2
−
1
	 é
⇒
	∝=
1
	 é
=
1
=
. é
2
= . 1
1+ 2
( ) = . (1 − ∝	
)
‫ج‬
-
‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫ﻋﺑﺎرة‬
( )
‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﺷﺣﻧﺔ‬ ‫وﻛذا‬
( )
:
( ) =
( )
=
( )
⇒ ( ) = 2. . 1
1+ 2
.
1
	 	 é
−∝	
( ) = Cé (1 −
	
)
⇒ ( ) =
	 	
−
	
= 0
−

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S22
 

Phx46

  • 1. ‫اﻟﺸﻌﺒﻴﺔ‬ ‫اﻃﻴﺔ‬‫ﺮ‬‫اﻟﺪﻳﻤﻘ‬ ‫ﻳﺔ‬‫ﺮ‬‫اﺋ‬‫ﺰ‬‫اﻟﺠ‬ ‫ﻳﺔ‬‫ر‬‫اﻟﺠﻤﻬﻮ‬ ‫ﻣﺴﺘﻐﺎﻧﻢ‬ ‫ﻟﻮﻻﻳﺔ‬ ‫ﺑﻴﺔ‬‫ﺮ‬‫اﻟﺘ‬ ‫ﻳﺔ‬‫ﺮ‬‫ﻣﺪﻳ‬ ‫ﻋﺸﻌﺎﺷﺔ‬ ‫ﺛﺎﻧﻮﻳﺔ‬ ) ‫اﻟﻘﺎدر‬ ‫ﻋﺒﺪ‬ ‫ﻳﻒ‬‫ﺮ‬‫ﺷ‬ ‫ﲪﺪي‬ ( ‫اﻷول‬ ‫اﻟﻔﺼﻞ‬ ‫اﻣﺘﺤﺎن‬ ‫اﺳﻴﺔ‬‫ر‬‫اﻟﺪ‬ ‫اﻟﺴﻨﺔ‬ : 2016 / 2017 ‫اﻟﺸﻌﺒﺔ‬ : ‫ﻳﺎﺿﻴﺎت‬‫ر‬ ‫اﻟﻤﺴﺘﻮى‬ : ‫اﻟﺜﺎﻟﺜﺔ‬ ‫اﻟﺴﻨﺔ‬ ‫ﻣﺎدة‬ ‫ﻓﻲ‬ ‫اﺧﺘﺒﺎر‬ : ‫ﻳﺎﺋﻴﺔ‬‫ﺰ‬‫اﻟﻔﻴ‬ ‫اﻟﻌﻠﻮم‬ ‫اﻟﻤﺪة‬ : 03 ‫ﺳﺎﻋﺎت‬ ‫أﺳﻮد‬ ‫أو‬ ‫أزرق‬ ‫ﺑﻘﻠﻢ‬ ‫إﺟﺎﺑﺘﻪ‬ ‫ﻳﺮ‬‫ﺮ‬‫ﺗﺤ‬ ، ‫اﻟﺘﻠﻤﻴﺬ‬ ‫ﻋﻠﻰ‬ : ‫ﻣﻼﺣﻈﺔ‬ ‫اﻷول‬ ‫اﻟﺗﻣرﯾن‬ : ) ,0 5 0 ‫ﻧﻘطﺔ‬ ( ‫اﻟﻧظﯾر‬ ‫ﯾﻌﺗﺑر‬ ‫ﺑﯾن‬ ‫ﻣن‬ ‫ﻟﻠﺗﻛﻧﺳﯾوم‬ ‫اﻟﻣﺷﻌﺔ‬ ‫اﻷﻧوﯾﺔ‬ ّ‫ﺑ‬‫اﻟط‬ ‫اﻟﻣﺟﺎل‬ ‫ﻓﻲ‬ ‫اﻟﻣﺳﺗﻌﻣﻠﺔ‬ ‫ﺧطورﺗﮫ‬ ‫وﻗﻠﺔ‬ ، ‫اﻟﻘﺻﯾرة‬ ‫ﺣﯾﺎﺗﮫ‬ ‫ﻟﻣدة‬ ‫اﻋﺗﺑﺎرا‬ ‫ﻲ‬ ‫اﻷطﺑﺎء‬ ‫إﺷﺎرة‬ ‫رھن‬ ‫وﺿﻌﮫ‬ ‫وﺳﮭوﻟﺔ‬ ‫اﻟﻣﻧﺧﻔﺿﺔ‬ ‫وﺗﻛﻠﻔﺗﮫ‬ ‫اﻹﺷﻌﺎﻋﯾﺔ‬ . 1 ( ‫ﯾﻌﺗﺑر‬ ‫و‬ ‫ﻟﻠﺗﻛﻧﯾﺳﯾوم‬ ‫ﻧظﯾران‬ . 1 - 1 ( ‫و‬ ‫اﻟﻣﺷﻌﺔ‬ ‫اﻟﻧواة‬ ‫ف‬ّ‫ﻋر‬ ‫اﻟﻧظﯾر‬ ‫ﻧواة‬ ‫ﺗرﻛﯾب‬ ‫اﻋط‬ . 1 - 2 ( ‫اﺳﺗﻘرارا‬ ‫اﻷﻛﺛر‬ ‫اﻟﻧواة‬ ‫اﻟﺗﻌﻠﯾل‬ ‫ﻣﻊ‬ ‫ّد‬‫د‬‫ﺣ‬ . 1 - 3 ( ‫اﻟﺗﻛﻧﺳﯾوم‬ ‫ﯾﻧﺗﺞ‬ ‫اﻟﻣوﻟﯾﺑدان‬ ‫ﻧواة‬ ‫ﺗﻔﻛك‬ ‫ﻋن‬ ( è ) . ‫أ‬ - ‫اﻟﺗﻛﻧﺗﯾوم‬ ‫ﻹﻧﺗﺎج‬ ‫اﻟﻧووي‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫أﻛﺗب‬ ‫اﻟﻣوﻟﯾﺑدان‬ ‫ﻣن‬ ‫اﻧطﻼﻗﺎ‬ . ‫؟‬ ‫اﻟﺣﺎﺻل‬ ‫اﻟﺗﻔﻛك‬ ‫ﻧﻣط‬ ‫ﻣﺎھو‬ ‫ب‬ - ‫اﻟﻣﺗﺣررة‬ ‫اﻟطﺎﻗﺔ‬ ‫أﺣﺳب‬ ‫اﻟﺣﺎدث‬ ‫اﻟﻧووي‬ ‫اﻟﺗﺣول‬ ‫ﯾواﻓق‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫ﻣﺧططﺎ‬ ‫أﻧﺟز‬ ℓ ‫ذﻟك‬ ‫ﺧﻼل‬ . 2 ( ‫اﻟﺗﻛﻧﺳﯾوم‬ ‫ﯾﺳﺗﻌﻣل‬ ‫ﺑﺟرﻋﺔ‬ ‫اﻹﻧﺳﺎن‬ ‫ﺟﺳم‬ ‫ﺣﻘن‬ ‫ﯾﺗم‬ ‫ﺣﯾث‬ ، ‫ﺗﺷﺧﯾﺻﮭﺎ‬ ‫ﻗﺻد‬ ‫اﻹﻧﺳﺎن‬ ‫ﻟﻌظﺎم‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫ﺑﺎﻟﻧﺷﺎط‬ ‫اﻟﺗﺻوﯾر‬ ‫ﻓﻲ‬ ‫اﻟﻣﺷﻊ‬ ‫اﻟﺗﻛﻧﯾﺗﯾوم‬ ‫ﻋﻠﻰ‬ ‫ﺗﺣﺗوي‬ ‫اﻟﻣﻔﺣوﺻﺔ‬ ‫ﻟﻠﻌظﺎم‬ ‫ﺻورة‬ ‫ﻋﻠﻰ‬ ‫ﻟﻠﺣﺻول‬ ‫زﻣﻧﯾﺔ‬ ‫ﻣدة‬ ‫ﺑﻌد‬ ‫ُﺳﺗﻛﺷف‬‫ﯾ‬ ‫واﻟذي‬ . ‫ﻓﻲ‬ ‫ﻧﻌطﻲ‬ ‫اﻟﺷﻛل‬ - 1 - ‫اﻷ‬ ‫ﻋدد‬ ‫ﺑدﻻﻟﺔ‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﻟﺗﻐﯾرات‬ ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫اﻟﻣﺗﻔﻛﻛﺔ‬ ‫ﻧوﯾﺔ‬ = ( ) . 2 - 1 ( ‫أ‬ - ‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫أوﺟد‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬  ‫ﻟﻠﺗﻛﻧﯾﺳﯾوم‬ . ‫ب‬ - ‫ھﻲ‬ ‫ﻟﮫ‬ ‫اﻟﻌﻣر‬ ‫ﻧﺻف‬ ‫زﻣن‬ ‫ﻗﯾﻣﺔ‬ ّ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬ : ½ = . ‫ﻋﻧد‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫ﻧﺷﺎطﮭﺎ‬ ‫ﺑﺣﻘﻧﺔ‬ ‫إﻧﺳﺎن‬ ‫ﺟﺳم‬ ‫ﺣﻘن‬ ‫ﺗم‬ = 0 ‫ھو‬ ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ‫اﻟﻣﻔﺣوﺻﺔ‬ ‫ﻟﻠﻌظﺎم‬ ‫ﺻورة‬ ‫أﺧذ‬ ‫ﻟﯾﺗم‬ ‫ﺗﺻﺑﺢ‬ ‫ﺣﯾث‬ ‫ﻋﻧدھﺎ‬ ‫اﻹﺷﻌﺎﻋﻲ‬ ‫اﻟﻧﺷﺎط‬ ‫ﻗﯾﻣﺔ‬ t ‫ھو‬ 60% ‫ﻗﯾﻣﺔ‬ ‫ﻣن‬ . 2 - 2 ( ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬ ‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬ ‫ﺑﮭﺎ‬ ‫اﻟﺟﺳم‬ ‫ﺣﻘن‬ ‫ﺗم‬ ‫اﻟﺗﻲ‬ ‫اﻟﻣﺷﻌﺔ‬ ‫اﻷﻧوﯾﺔ‬ ‫ﻋدد‬ = 0 . 2 - 3 - ( ‫ﺑﺎﻟﺳﺎﻋﺔ‬ ‫ﺣدد‬ ) ℎ ( ‫ﻗﯾﻣﺔ‬ . ‫اﻟﻣﻌطﯾﺎت‬ : 1 = 931,5 . ، = 1,0073 = 0,00055 ، = 1,0087 ‫اﻟﺼﻔﺤﺔ‬ 1 / 4 ‫اﻟﻧواة‬ ( ) ( ) ( ) ℓ( ) ℓ = 852,10 ℓ = 852,53 ℓ = 836,28
  • 2. ‫اﻟﺗﻣرﯾن‬ ‫اﻟﺛﺎﻧﻲ‬ : ) ,0 6 0 ‫ﻧﻘطﺔ‬ ( ‫ﻧﺿﻊ‬ ‫ﻛﺄس‬ ‫ﻓﻲ‬ ‫ﺣﺟﻣﺎ‬ ‫اﻟﺻودﯾوم‬ ‫ﻟﮭﯾدروﻛﺳﯾد‬ ‫ﻣﺎﺋﻲ‬ ‫ﻣﺣﻠول‬ ‫ﻣن‬ ) ( ) , ( ) ( ‫ﻣﺎدﺗﮫ‬ ‫ﻛﻣﯾﺔ‬ ‫اﻟﻣوﻟﻲ‬ ‫وﺗرﻛﯾزه‬ = 10 ℓ. ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ‫إﻟﯾﮫ‬ ‫ﻧﺿﯾف‬ ‫ﺛم‬ = 0 ‫اﻟﻣﺎدة‬ ‫ﻛﻣﯾﺔ‬ ‫ﻧﻔس‬ ، ‫ﺗﻔﺎﻋﻠﻲ‬ ‫ﺧﻠﯾط‬ ‫ﻋﻠﻰ‬ ‫ﻟﻧﺣﺻل‬ ‫اﻹﯾﺛﯾل‬ ‫إﯾﺗﺎﻧوات‬ ‫ﻣن‬ ‫ﺣﺟﻣﮫ‬ ‫اﻟﻣوﻻت‬ ‫ﻣﺗﺳﺎوي‬ ≈ = 10 . ‫ﻧﻧﻣذج‬ ‫ﺑﯾن‬ ‫ﯾﺣدث‬ ‫اﻟذي‬ ‫اﻟﻛﯾﻣﯾﺎﺋﻲ‬ ‫اﻟﺗﺣول‬ ‫اﻹﯾﺛﯾل‬ ‫إﯾﺗﺎﻧوات‬ ‫و‬ ‫اﻟﺻودﯾوم‬ ‫ﻟﮭﯾدروﻛﺳﯾد‬ ‫اﻟﺗﺎﻟﯾﺔ‬ ‫ﺑﺎﻟﻣﻌﺎدﻟﺔ‬ : (ℓ) + ( ) −→ ( ) + − ( ) 1 - ‫أ‬ - ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬ ‫واﺳﺗﻧﺗﺞ‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻟﺗﻘدم‬ ‫ﺟدوﻻ‬ ‫أﻧﺟز‬ . ‫ب‬ - ‫اﻟﺗﻔ‬ ‫ﻟﻠوﺳط‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻋﺑﺎرة‬ ‫أﻛﺗب‬ ‫ﺎﻋﻠﻲ‬ :  ) ‫ﻋﻧد‬ = 0 ( .  ( ) ) ‫ﻟﻣﺎ‬ > 0 ( ‫ﺑدﻻﻟﺔ‬ ، ، ،  ‫و‬  . ‫ج‬ - ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬ = ( ) ‫ا‬ ‫ﻟﺷﻛل‬ ) 2 ( ‫ﻋﺑﺎرة‬ ‫أﻛﺗب‬ ( ) ‫ﺑدﻻﻟﺔ‬ . ‫د‬ - ‫اﻟﺳؤاﻟﯾن‬ ‫ﺑﺈﺟﺎﺑﺔ‬ ‫ﺑﺎﻻﺳﺗﻌﺎﻧﺔ‬ ) ‫ب‬ – ‫ج‬ ( ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﺗﻧﺎﻗص‬ ‫ﺳﺑب‬ ‫ّن‬‫ﯾ‬‫ﺑ‬ ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫اﻟوﺳط‬ ‫ﻓﻲ‬ ‫اﻟﻧوﻋﯾﺔ‬ . 2 - ‫اﻟﻛﯾﻣﺎﺋﻲ‬ ‫اﻟﺗﺣول‬ ‫ﻟﺗطور‬ ‫اﻟزﻣﻧﯾﺔ‬ ‫اﻟﻣﺗﺎﺑﻌﺔ‬ : ‫ﺗطور‬ ‫ﻧﺗﺗﺑﻊ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻗﯾﺎس‬ ‫طرﯾق‬ ‫ﻋن‬ ‫اﻟﻛﯾﻣﺎﺋﻲ‬ ‫اﻟﺗﺣول‬ ‫ﺑواﺳطﺔ‬ ‫ﻟﻧﺣﺻل‬ ‫اﻟزﻣن‬ ‫ﺧﻼل‬ ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠﻣزﯾﺞ‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﺑﯾﺎﻧﻲ‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﻣﻌﻠوﻣﺎﺗﯾﺔ‬ ‫ﺑرﻣﺟﯾﺔ‬ = ( ) ‫اﻟﺷﻛل‬ ‫ﻓﻲ‬ ) 3 ( . 2 - 1 ( ‫أﺣﺳب‬ ½ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠﺧﻠﯾط‬ ‫ﺛم‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻧﺻف‬ ‫زﻣن‬ ‫اﺳﺗﻧﺗﺞ‬ ½ . 2 - 3 ( ‫اﻟﺗﻔﺎﻋل‬ ‫ﺣرﻛﯾﺔ‬ : ‫أ‬ ( ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﻋرف‬ ‫ﺑدﻻﻟﺔ‬ ‫ﻋﺑﺎرﺗﮭﺎ‬ ‫أوﺟد‬ ‫ﺛم‬ ( ) . ‫ب‬ - ‫ﺑﺎﻟوﺣدة‬ ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫أﺣﺳب‬ ) ℓ . . ( ‫اﻟﻠﺣظﺗﯾن‬ ‫ﻋﻧد‬ ) : = 0 ( ‫و‬ ) = 35 ( . ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﺗطور‬ ‫اﺷرح‬ . ‫ﻣﻌطﯾﺎت‬ : ‫اﻟﺷﺎردة‬ ( ) ( ) ( ) ‫ﺑـ‬ ‫اﻟﺷﺎردﯾﺔ‬ ‫اﻟﻣوﻟﯾﺔ‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ى‬ ) . . (    ‫اﻟﺼﻔﺤﺔ‬ 2 / 4
  • 3. ‫اﻟﺗﻣرﯾن‬ ‫اﻟﺛﺎﻟث‬ : ) 5 04, ‫ﻧﻘطﺔ‬ ( ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟدارة‬ ‫ﺗﻌﺗﺑر‬ ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻷﺟﮭزة‬ ‫ﻣن‬ ‫ﻟﻣﺟﻣوﻋﺔ‬ ‫اﻹﻟﻛﺗروﻧﯾﺔ‬ ‫اﻟﺗراﻛﯾب‬ ‫ﻓﻲ‬ ‫اﻟﻣﺳﺗﻌﻣﻠﺔ‬ ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟدارات‬ ‫ﺑﯾن‬ ‫ﻣن‬ . ‫ﻓﻲ‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺗرﻛﯾب‬ ‫ﯾﺗﻛون‬ ‫اﻟﺷﻛل‬ - 4 - ‫ﻣن‬ : - ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟﻣﺣرﻛﺔ‬ ‫ﻗوﺗﮫ‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﺛﺎﻟﻲ‬ ‫ﻣوﻟد‬ . - ‫ﺳﻌﺗﺎھﻣﺎ‬ ‫ﻣﻛﺛﻔﺗﯾن‬ ‫و‬ = 2 . - ‫ﻣﻘﺎوﻣﺗﮫ‬ ‫اوﻣﻲ‬ ‫ﻧﺎﻗل‬ = 3  . - ‫ﻟﻠﺗﯾﺎر‬ ‫ﻗﺎطﻌﺔ‬ . ‫ﻟﻸزﻣﻧﺔ‬ ‫ﻣﺑدءا‬ ‫ﻧﺧﺗﺎرھﺎ‬ ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ) = 0 ( ‫اﻟﻘﺎطﻌﺔ‬ ‫ﻧﻐﻠق‬ ، . 1 - ‫اﻟﺳﻌﺔ‬ ‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬ Cé ‫ھﻲ‬ ‫اﻟدارة‬ ‫ﻓﻲ‬ ‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫ﻟﻠﻣﻛﺛﻔﺔ‬ : 1. 2 1+ 2 Cé = . 2 - ‫أ‬ - ‫اﻟﺗوﺗر‬ ‫ﯾﺣﻘﻘﮭﺎ‬ ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬ ( ) ‫ذ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫طرﻓﻲ‬ ‫ﺑﯾن‬ ‫ات‬ ‫اﻟﺳﻌﺔ‬ ‫ﺗﻛﺗب‬ ‫ﺑﺎﻟﺷﻛل‬ : ( ) + é 2( ) = 2 ‫ب‬ - ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ھذه‬ ‫ﺣل‬ ‫ﯾﻛﺗب‬ ‫اﻟﺷﻛل‬ ‫ﻋﻠﻰ‬ : ( ) = (1 − ∝ ) . - ‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻣن‬ ‫ﻛل‬ ‫ﻋﺑﺎرة‬ ‫ﺣدد‬ ‫و‬ ∝ ‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬ . ‫ج‬ - ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫ﻋﺑﺎرة‬ ‫اوﺟد‬ ( ) ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﺷﺣﻧﺔ‬ ‫وﻛذا‬ ( ) . 3 - ‫ﯾﻣﺛل‬ ② ‫و‬ ① ‫ﻣﻧﺣﻧﯾﺎ‬ ‫اﻟﺷﻛل‬ – 5 - ‫اﻟﻛﮭرﺑﺎﺋﯾﯾن‬ ‫اﻟﺗوﺗرﯾن‬ ‫ﺗطور‬ ( ) ‫و‬ ( ) . ‫أ‬ - ‫اﻟﺗﺑرﯾر‬ ‫ﻣﻊ‬ ‫اﻟﻣﻧﺎﺳب‬ ‫ﻟﻠﺗوﺗر‬ ‫ﺑﯾﺎﻧﻲ‬ ‫ﻣﻧﺣﻧﻰ‬ ‫ﻛل‬ ‫أﻧﺳب‬ . ‫ب‬ - ‫اﻟﺗوﺗر‬ ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫وأﺣﺳب‬ . ‫ج‬ - ‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫ﺑﯾﺎﻧﯾﺎ‬ ‫أوﺟد‬ ‫ﺛم‬ ‫أن‬ ‫ّن‬‫ﯾ‬‫ﺑ‬ : = 4 . 4 - ‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫اﻷﻋظﻣﯾﺔ‬ ‫اﻟﻘﯾﻣﺔ‬ ‫أﺣﺳب‬ . ‫اﻟراﺑﻊ‬ ‫اﻟﺗﻣرﯾن‬ : ) 5 , 4 0 ‫ﻧﻘطﺔ‬ ( ‫ﻓﻲ‬ ‫اﻟﻣﺑﯾن‬ ‫اﻟﺗرﻛﯾب‬ ‫ﻧﻧﺟز‬ ‫اﻟﺷﻛل‬ - 6 - ‫ﻣن‬ ‫واﻟﻣﻛون‬ : - ‫اﻟﻛﮭرﺑﺎﺋﯾﺔ‬ ‫اﻟﻣﺣرﻛﺔ‬ ‫ﻗوﺗﮫ‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﺛﺎﻟﻲ‬ ‫ﻣوﻟد‬ = 12 - ‫وﺷﯾﻌﺔ‬ ‫ﻣﺛﺎﻟﯾﺔ‬ ‫ﺗﺣرﯾﺿﮭﺎ‬ ‫ﻣﻌﺎﻣل‬ ) ‫ذاﺗﯾﺗﮭﺎ‬ ( . - ‫اوﻣﯾﯾن‬ ‫ﻧﺎﻗﻠﯾن‬ ‫ﻣﻘﺎوﻣﺎﺗﮭﻣﺎ‬ = 40 ‫و‬ - ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫ﻟﻠﺗﯾﺎر‬ ‫ﻗﺎطﻌﺔ‬ . ‫اﻟﺼﻔﺤﺔ‬ 3 / 4
  • 4. ‫ﻟﻸزﻣﻧﺔ‬ ‫ﻣﺑدءا‬ ‫ﻧﺧﺗﺎرھﺎ‬ ‫ﻟﺣظﺔ‬ ‫ﻋﻧد‬ ) = 0 ( ‫اﻟﻘﺎطﻌﺔ‬ ‫ﻧﻐﻠق‬ ، ‫ﺑﺎﻟدارة‬ ‫ﻣوﺻل‬ ‫ﻣﻌﻠوﻣﺎﺗﻲ‬ ‫ﻧظﺎم‬ ‫وﺑواﺳطﺔ‬ ) ‫ﯾظﮭر‬ ‫ﻻ‬ ‫اﻟدارة‬ ‫ﻓﻲ‬ ( ‫اﻟﻣﻧﺣﻧﯾﯾن‬ ‫ﻋﻠﻰ‬ ‫ﻧﺣﺻل‬ ( ) ‫و‬ ( ) ‫اﻟﻣدﺧﻠﯾن‬ ‫ﻋﻧد‬ ‫ﻟﻠﺗوﺗرﯾن‬ ‫اﻟﻣﻣﺛﻠﯾن‬ A ‫و‬ B ‫اﻟﺷﻛل‬ - 7 - . 1 - ‫اﻟﺗوﺗر‬ ‫ﯾﻣﺛل‬ ‫اﻟذي‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ّن‬‫ﯾ‬‫ﻋ‬ ( ) ‫اﻟﺗوﺗر‬ ‫ﯾﻣﺛل‬ ‫اﻟذي‬ ‫واﻟﻣﻧﺣﻧﻰ‬ ( ) . 2 - ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬ ‫اﻟداﺋم‬ ‫اﻟﻧظﺎم‬ ‫ﻓﻲ‬ ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ، . 3 - ‫اﻟﻣﻘﺎوﻣﺔ‬ ‫ﻗﯾﻣﺔ‬ ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬ ‫ﻟﻠﻧﺎﻗل‬ ‫اﻷوﻣﻲ‬ ‫ھﻲ‬ = 8  . 4 - ‫أﺛﺑت‬ ‫اﻟﺗوﺗرات‬ ‫ﺟﻣﻊ‬ ‫ﻗﺎﻧون‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬ ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗوﺗر‬ ‫ﯾﺣﻘﻘﮭﺎ‬ ( ) . 5 - ‫اﻟﺷﻛل‬ ‫ﻣن‬ ‫ھو‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﺣل‬ ‫أن‬ ‫ﻋﻠﻣﺎ‬ : (1 − ) ( ) = . ‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻋﺑﺎرﺗﻲ‬ ‫أوﺟد‬ ‫و‬ ‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬ . 6 - ‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫ﺣدد‬ ‫ﻟﻠدارة‬ . 7 - ‫اﻟﺗﺣرﯾض‬ ‫ﻣﻌﺎﻣل‬ ‫ﻗﯾﻣﺔ‬ ‫اﺳﺗﻧﺗﺞ‬ ‫ﻟﻠوﺷﯾﻌﺔ‬ . 8 - ‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬ ‫اﻟوﺷﯾﻌﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫اﻟطﺎﻗﺔ‬ ‫أﺣﺳب‬ = . ‫اﻟﺼﻔﺤﺔ‬ 4 / 4
  • 5. ‫ﻋﺒﺪاﻟﻘﺎدر‬ ‫ﻳﻒ‬‫ﺮ‬‫ﺷ‬ ‫ﺣﻤﺪي‬ ‫ﺛﺎﻧﻮﻳﺔ‬ – ‫ﻋﺸﻌﺎﺷﺔ‬ - ‫ﻟﻤﺎدة‬ ‫اﻷول‬ ‫اﻟﻔﺼﻞ‬ ‫اﻣﺘﺤﺎن‬ ‫ﺗﺼﺤﻴﺢ‬ ‫ﻳﺎﺋﻴﺔ‬‫ﺰ‬‫اﻟﻔﻴ‬ ‫اﻟﻌﻠﻮم‬ – ‫اﻟﺜﺎ‬ ‫اﻟﺴﻨﺔ‬ ‫ﻟﺜﺔ‬ ‫ﺷﻌﺒ‬ ‫ﺔ‬ ) ‫ﻳﺎﺿﻴﺎت‬‫ر‬ ( ‫اﺳﻴﺔ‬‫ر‬‫اﻟﺪ‬ ‫اﻟﺴﻨﺔ‬ : 2016 - 2017 ‫د‬ - ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﺗﻧﺎﻗص‬ ‫ﺳﺑب‬ ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫اﻟوﺳط‬ ‫ﻓﻲ‬ ‫اﻟﻧوﻋﯾﺔ‬ . ‫اﻟﻌﻼﻗﺗﯾن‬ ‫ﺑﻣطﺎﺑﻘﺔ‬  ‫و‬  :  −  < 0 ⇒  <  2 - 1 ( ‫ﺣﺳ‬ ‫ﺎ‬ ‫ب‬ ½ ‫اﺳﺗﻧﺗ‬ ‫ﺛم‬ ‫ﺎ‬ ‫ج‬ ½ . σ½ = 0,25 − 160 2 ⇒ σ½ = 0,17 . −1 = 170 . −1 ⟹ ½ = 12 2 - 1 - ‫اﻟﺗﻔﺎﻋل‬ ‫ﺣرﻛﯾﺔ‬ : ‫أ‬ ( ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﺑدﻻﻟﺔ‬ ‫ﻋﺑﺎرﺗﮭﺎ‬ ( ) : ‫واﺣدة‬ ‫ﻓﻲ‬ ‫اﻟزﻣن‬ ‫ﺧﻼل‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﺗﻘدم‬ ‫ﺗﻐﯾرات‬ ‫ﻣﻘدار‬ ‫ھﻲ‬ ‫وﻧﻛﺗب‬ ‫اﻟﺣﺟوم‬ : = = − , ‫ب‬ - ‫ﺣﺳ‬ ‫ﺎ‬ ‫ب‬ ‫ﺑﺎﻟوﺣدة‬ ) ℓ . . ( ‫ﻋﻧد‬ ‫اﻟﻠﺣظﺗﯾن‬ ) : = 0 ( ‫و‬ ) = 35 . ( = × ‖ ‖ ‖ ‖ (0) = 0,52 ℓ . . (35min) = 0,083 ℓ . . ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻟﺣﺟﻣﯾﺔ‬ ‫اﻟﺳرﻋﺔ‬ ‫ﺗطور‬ ‫ﺷرح‬ . (0) > (35min) ‫ﺧﻼل‬ ‫اﻟﻣﺗﻔﺎﻋﻼت‬ ‫ﺗراﻛﯾز‬ ‫ﺗﻧﺎﻗص‬ ‫ﺑﺑﺳﺑب‬ ‫ﺗﺗﻧﺎﻗص‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﺳرﻋﺔ‬ ‫اﻟزﻣن‬ . ‫ﻧﺟد‬ ‫ﺑﺎﻟﻣطﺎﺑﻘﺔ‬ : = . = = 5. 10 Bq  = − = × ‖ ‖ ‖ ‖ = 3,22. 10 ‫ب‬ - ّ‫أن‬ ‫ﻣن‬ ‫ﺗﺣﻘق‬ ½ = : ½ = ℓ  = , . ≈ 2 - 2 - ‫ﻗﯾﻣﺔ‬ ‫اﻟﻠﺣظﺔ‬ ‫ﻋﻧد‬ = 0 : = . ⇒ =  = 1,55. 10 2 - 3 - ‫ﺗ‬ ‫ﺣد‬ ‫ﯾ‬ ‫ﺑﺎﻟﺳﺎﻋﺔ‬ ‫د‬ ) ℎ ( ‫ﻗﯾﻣﺔ‬ : = 0. − ⇒ 0,60 =  ⇒ =  ℓ 0 = 4,4 ℎ ‫اﻟﺛﺎﻧﻲ‬ ‫اﻟﺗﻣرﯾن‬ 06 ‫ﻧﻘط‬ : 1 - ‫أ‬ - ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬ ‫واﺳﺗﻧﺗﺞ‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻟﺗﻘدم‬ ‫ﺟدوﻻ‬ ‫أﻧﺟز‬ . ‫ﻟﻠﺗﻔﺎﻋل‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﺗﻘدم‬ : − = 0 ⟹ = = = 10 ℓ ‫ب‬ - ‫اﻟﺗﻔﺎﻋﻠﻲ‬ ‫ﻟﻠوﺳط‬ ‫اﻟﻧوﻋﯾﺔ‬ ‫اﻟﻧﺎﻗﻠﯾﺔ‬ ‫ﻋﺑﺎرة‬ : =  [ ] +  [ ] ⟹ = ( +  ) ( ) =  [ ] +  [ ] +  2 3 2( ) − ( ) =  +  +  = ( +  ) + ( −  )  ……………… ( ) = + ( −  ) ‫ج‬ - ‫ﻋﺑﺎرة‬ ( ) ‫ﺑدﻻﻟﺔ‬ . ( ) = + = = 0,25 . = × ‖ ‖ ‖ ‖ ≈ −160 / . ℓ.  … ………………… ⇒ ( ) = 0,25 − 160 (ℓ) + ( ) −→ ( ) + − ( ) ‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬ ‫ﺑـ‬ ‫اﻟﻣﺎدة‬ ‫ﻛﻣﯾــــــــــﺎت‬ ( ℓ) ‫اﻟﺗﻘدم‬ ‫اﻟ‬ ‫ﺣﺎﻟﺔ‬ 0 0 ‫إﺑﺗدا‬ − − ‫اﻧﺗﻘﺎ‬ − − ‫ﻧﮭﺎ‬ ‫اﻷول‬ ‫اﻟﺗﻣرﯾن‬ : 06 ‫ﻧﻘطﺔ‬ 1 - 1 ( ‫اﻟﻧظﯾر‬ ‫ﻧواة‬ ‫ﺗرﻛﯾب‬ : 43 + 56 1 - 2 ( ‫اﻟﺗﻌﻠﯾل‬ ‫ﻣﻊ‬ ‫اﺳﺗﻘرارا‬ ‫اﻷﻛﺛر‬ ‫اﻟﻧواة‬ . ℓ = 8,621 / é ℓ = 8,611 / é ‫اﻟﻧواة‬ ‫اﻟﻧواة‬ ‫ﻣن‬ ‫اﺳﺗﻘرارا‬ ‫أﻛﺛر‬ ‫ﻷن‬ ⇒ ℓ > ℓ 3 - ‫أ‬ - ‫اﻟﺗﻛﻧﺗﯾوم‬ ‫ﻹﻧﺗﺎج‬ ‫اﻟﻧووي‬ ‫اﻟﺗﻔﺎﻋل‬ ‫ﻣﻌﺎدﻟﺔ‬ . ⟶ + ‫ﺻودي‬ ‫ﻗﺎﻧوﻧﻲ‬ ‫ﺣﺳب‬ 99 = 99 + 42 = 43 + ⇒ = 0 = −1 ⟹ ⇛ ‫اﻟﺗﻔﻛك‬ ‫ﻧﻣط‬ : ) ‫اﻟﻛﺗرون‬ ( ⟶ + ‫ب‬ - ‫وﺣﺳ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫ﻣﺧطط‬ ‫ﺎ‬ ‫اﻟﻣﺗﺣررة‬ ‫اﻟطﺎﻗﺔ‬ ‫ب‬ ℓ : ℓ = − ℓ + + − . − ℓ ℓ = −[852,10 + (1,0073 + 0,00055 − 1,0087).931,5 − 852,53] = 737,96 2 - 1 ( ‫أ‬ - ‫اﻟﻣﻧﺣﻧﻰ‬ ‫ﻋﻠﻰ‬ ‫ﺑﺎﻻﻋﺗﻣﺎد‬ = ( ) ‫إﯾﺟﺎد‬  ‫ﻟـ‬ . ‫ﻟدﯾﻧﺎ‬ : ( ) =  ( ) = . − . … … … … . ‫ ﻧظرﯾﺎ‬ ( ) = + . … … … … … … … … . . … . ‫ ﺑﯾﺎﻧﯾﺎ‬
  • 6. ⇒ = − ( ) ⇒ = 12 − 10 0,25 = 8  4 - ‫ﺗﺣﻘﻘﮭﺎ‬ ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ( ) : ∀ ≥ 0 ∶ ( ) + ( ) + ( ) = ( ) = ( ) = ( ) ⇒ ( ) = ( ) ( ) = ( ) ⇒ ( ) + ( ) + ( ) = ⟹ ( ) + ( ) ( ) = 5 - ‫اﻟﺷﻛل‬ ‫ﻣن‬ ‫ھو‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ﺣل‬ : . (1 − ) ( ) = - ‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻋﺑﺎرﺗﻲ‬ ‫إﯾﺟﺎد‬ : ‫و‬ ( ) = A. A. + ( ) − ( ) = ⇒ ( + ) = = ( ) ⇒ = ( ) = = ( ) 6 - ‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻗﯾﻣﺔ‬ ‫ﻟﻠدارة‬ : ‫اﻟﺑﯾﺎن‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬ ( ‫ﻧﺣﺳب‬ : ( ) = 0,63 (max) = 6,3 ⇒ = 7 - ‫اﻟﺗﺣرﯾض‬ ‫ﻣﻌﺎﻣل‬ ‫ﻗﯾﻣﺔ‬ ‫ﻟﻠوﺷﯾﻌﺔ‬ : = ( ) ⇒ = ( + ) ⇒ = 8 - ‫اﻟطﺎ‬ ‫أﺣﺳب‬ ‫ﻋﻧد‬ ‫اﻟوﺷﯾﻌﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻗﺔ‬ : = ( ) = ½ ( ) ⇒ ( )⌋ = = ½ ( ) = = 1,5 ⇒ = 4 ⇒ = , ( )⌋ = , . . , ⇒ ( )⌋ = , 3 - ‫أ‬ - ‫اﺳ‬ ‫ﻧﺎد‬ ‫اﻟﺗﺑرﯾر‬ ‫ﻣﻊ‬ ‫اﻟﻣﻧﺎﺳب‬ ‫ﻟﻠﺗوﺗر‬ ‫ﻣﻧﺣﻧﻰ‬ ‫ﻛل‬ . (0) = 0 ( ) = 0 ⇒ (0) = ( ) = 0 ‫اﻟﻣﻧﺣﻧﻰ‬  ‫ﻟﻠﺗوﺗر‬ ( ) 2(0) = 0 2( ) = . ‫اﻟﻣﻧﺣﻧﻰ‬  ‫ﻟﻠﺗوﺗر‬ ( ) ‫ب‬ - ‫اﻟﺗوﺗر‬ ‫ﻗﯾﻣﺔ‬ ‫اﻷﻋظﻣﻲ‬ ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫وﺣﺳﺎب‬ : = (0) = = . = ⇒ = 12 = 4. 10 ‫ج‬ - ‫ﺗ‬ ّ‫ﯾ‬‫ﺑ‬ ‫ﺎ‬ ‫أن‬ ‫ن‬ : = : ‫ﺑﯾﺎﻧﯾﺎ‬ ‫اﻟزﻣن‬ ‫ﺛﺎﺑت‬ ‫ﻧﺣﺳب‬ : ‫اﻟﺑﯾﺎن‬ ‫ﺑﺎﺳﺗﻌﻣﺎل‬  ⇒ = 4 ( ) = 0,37 = 4,44 = é ⇒ é = ⇒ é = 4 3 + = é ⇒ = é − = ⇒ C = 4 μ F 4 - ‫ﺣﺳ‬ ‫ﺎ‬ ‫اﻟﻣﻛﺎﻓﺋﺔ‬ ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﻓﻲ‬ ‫اﻟﻣﺧزﻧﺔ‬ ‫ﻟﻠطﺎﻗﺔ‬ ‫اﻷﻋظﻣﯾﺔ‬ ‫اﻟﻘﯾﻣﺔ‬ ‫ب‬ : ( ) = ½Cé 2 = ½ . 2 ( ) = 3 8 . 144 = 54 ‫اﻟﺗﻣرﯾن‬ ‫اﻟراﺑﻊ‬ : ) 0 0 . 4 ‫ﻧﻘطﺔ‬ ( 1 - ‫اﻟﻣﻧﺣﻧﯾﯾن‬ ‫اﺳﻧﺎد‬ : ∀ ≥ 0 ∶ ( ) = − ( ) ( ) = ( ) (0) = , ( ) = − (0) = 0) = 0 , ( ) = ‫اﻟﻣﻧﺣﻧﻰ‬ ‫وﻣﻧﮫ‬ ( ) ‫ﯾواﻓق‬ ( ) ‫و‬ ‫اﻟﻣﻧﺣﻧﻰ‬ ( ) ‫ﻟـ‬ ( ) 2 - ‫ﻗﯾﻣﺔ‬ : ( ) = ( ) = 10 ⇒ = ( ) = = 0,25 3 - ‫اﻟﻣﻘﺎوﻣﺔ‬ ‫ﻗﯾﻣﺔ‬ ‫أن‬ ‫ﻣن‬ ‫اﻟﺗﺣﻘق‬ ‫ھﻲ‬ ‫اﻷوﻣﻲ‬ ‫ﻟﻠﻧﺎﻗل‬ =  . ‫اﻟﺛﺎﻟث‬ ‫اﻟﺗﻣرﯾن‬ : ) 0 0 . 4 ‫ﻧﻘطﺔ‬ ( =? ‫و‬ = 2 . =? = 3  1 - ‫ﺗﺑﯾﺎن‬ ‫أن‬ : 1. 2 1+ 2 Cé = . = = + = + = é ⇒ 1 C1 + 1 C2 = 1 é ⇒ Cé = 1. 2 1+ 2 2 - ‫أ‬ - ‫اﻟﺗﻲ‬ ‫اﻟﺗﻔﺎﺿﻠﯾﺔ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ( ) : ( ) + é 2( ) = 2 ∀ ≥ 0 ∶ ( ) + ( ) + ( ) = ‫اﻟﺗوﺗرات‬ ‫ﺟﻣﻊ‬ ‫ﻗﺎﻧون‬ ( ) = = = ( ) ( ) = é − ⇒ ( ) + é =  …………. ⟹ ( ) + é ( ) = ‫ب‬ - ‫اﻟﺷﻛل‬ ‫ﻋﻠﻰ‬ ‫اﻟﻣﻌﺎدﻟﺔ‬ ‫ھذه‬ ‫ﺣل‬ : ( ) = (1 − ∝ ) . ‫اﻟﺛﺎﺑﺗﯾن‬ ‫ﻣن‬ ‫ﻛل‬ ‫ﻋﺑﺎرة‬ ‫و‬ ∝ ‫ﻟﻠدارة‬ ‫اﻟﻣﻣﯾزة‬ ‫اﻟﻣﻘﺎدﯾر‬ ‫ﺑدﻻﻟﺔ‬ 2 = A ∝ −∝ ‫ﻓﻲ‬ ‫ﺑﺎﻟﺗﻌوﯾض‬  : ⇒ A ∝ ∝ + é − é A ∝ = ⇒ A ∝ ∝ − é = − é ∝ − 1 é = 0 2 − 1 é ⇒ ∝= 1 é = 1 = . é 2 = . 1 1+ 2 ( ) = . (1 − ∝ ) ‫ج‬ - ‫اﻟﻛﮭرﺑﺎﺋﻲ‬ ‫اﻟﺗﯾﺎر‬ ‫ﺷدة‬ ‫ﻋﺑﺎرة‬ ( ) ‫اﻟﻣﻛﺛﻔﺔ‬ ‫ﺷﺣﻧﺔ‬ ‫وﻛذا‬ ( ) : ( ) = ( ) = ( ) ⇒ ( ) = 2. . 1 1+ 2 . 1 é −∝ ( ) = Cé (1 − ) ⇒ ( ) = − = 0 −