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‫ﺍﻷﻭﻝ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬
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‫ﺍﻻﻨﺩﻤﺎﺝ‬ ‫ﺘﻔﺎﻋﻝ‬
‫ﺘﺴـﺨﻴﻥ‬ ‫ﻀـﺭﻭﺭﺓ‬ :‫ﺒﻴﻨﻬﺎ‬ ‫ﻤﻥ‬ ‫ﺘﻘﻨﻴﺔ‬ ‫ﺼﻌﻭﺒﺎﺕ‬ ‫ﻋﺩﺓ‬ ‫ﻴﻁﺭﺡ‬ ‫ﺇﻨﺠﺎﺯﻩ‬ ‫ﻟﻜﻥ‬ ،‫ﻟﻠﺤﺭﺍﺭﺓ‬ ‫ﻨﺎﺸﺭ‬ ‫ﺘﻔﺎﻋﻝ‬ ‫ﺍﻟﻨﻭﻭﻱ‬
‫ﺘﻔﻭﻕ‬ ‫ﻋﺎﻟﻴﺔ‬ ‫ﺤﺭﺍﺭﺓ‬ ‫ﺩﺭﺠﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺨﻠﻴﻁ‬
ͳͲͲ
.‫ﺍﻟﺘﻔﺎﻋﻝ‬ ‫ﺍﻨﻁﻼﻕ‬ ‫ﻟﻀﻤﺎﻥ‬ ‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬
‫ﻤ‬
‫ﺒ‬ ‫ﻥ‬
‫ﻴ‬
‫ﺍﻻﻨﺩﻤ‬ ‫ﺘﻔﺎﻋﻼﺕ‬ ‫ﻥ‬
‫ـ‬
‫ﺎﺝ‬
،
‫ﺍﻟﻨﻅﻴ‬ ‫ﺍﻨﺩﻤﺎﺝ‬
‫ـ‬
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺭﻴﻥ‬
‫ܪ‬
ଵ
ଶ
‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬
‫ܪ‬
ଵ
ଷ
‫ﺍﻟﻬﻴﻠﻴ‬ ‫ﻨﻭﺍﺓ‬ ‫ﻴﻌﻁﻲ‬ ‫ﺍﻟﺫﻱ‬ ‫ﻭ‬
‫ـ‬
‫ﻭﻡ‬
‫݁ܪ‬
ଶ
ସ
‫ﻨﺘﺭﻭﻥ‬ ‫ﻭ‬
݊
଴
ଵ
.
ͳ
-
.‫ﺍﻟﻨﻅﺎﺌﺭ‬ ،‫ﺍﻟﻨﻭﻭﻱ‬ ‫ﺍﻻﻨﺩﻤﺎﺝ‬ :‫ﻴﻠﻲ‬ ‫ﻤﺎ‬ ‫ﻑ‬
‫ﺭ‬‫ﻋ‬
ʹ
-
‫ﺘﻔﻭﻕ‬ ‫ﻋﺎﻟﻴﺔ‬ ‫ﺤﺭﺍﺭﺓ‬ ‫ﺩﺭﺠﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺨﻠﻴﻁ‬ ‫ﺘﺴﺨﻴﻥ‬ ‫ﻴﺘﻡ‬ ‫ﻟﻤﺎﺫﺍ‬ ‫ﺍﺸﺭﺡ‬
ͳͲͲ
.‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬
͵
-
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺍﻟﻨﻅﻴﺭﻴﻥ‬ ‫ﺒﻴﻥ‬ ‫ﺍﻟﻨﻭﻭﻱ‬ ‫ﺍﻻﻨﺩﻤﺎﺝ‬ ‫ﻤﻌﺎﺩﻟﺔ‬ ‫ﺍﻜﺘﺏ‬
‫ܪ‬
ଵ
ଶ
‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬
‫ܪ‬
ଵ
ଷ
.
Ͷ
-
‫ﺒﺎﻟـ‬ ‫ﺍﺤﺴﺏ‬
‡
‫ﺒﺎﻟـ‬ ‫ﺜﻡ‬

‘—Ž
.‫ﺍﻟﺘﻔﺎﻋﻝ‬ ‫ﻫﺫﺍ‬ ‫ﺭﻫﺎ‬
‫ﺭ‬‫ﻴﺤ‬ ‫ﺍﻟﺘﻲ‬ ‫ﺍﻟﻁﺎﻗﺔ‬
ͷ
-
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻴﻭﺠﺩ‬
‫ܪ‬
ଵ
ଶ
‫ﺒــ‬ ‫ﻤﻨﻪ‬ ‫ﺍﻟﻌﺎﻟﻤﻲ‬ ‫ﺍﻻﺤﺘﻴﺎﻁ‬ ‫ﺭ‬
‫ﺩ‬‫ﻴﻘ‬ ‫ﺤﻴﺙ‬ ،‫ﺍﻟﻤﺤﻴﻁﺎﺕ‬ ‫ﻓﻲ‬ ‫ﺒﻭﻓﺭﺓ‬
‰

ͳ͸
Ͷǡ͸šͳͲ
‫ﻫـﻭ‬ ‫ﻭ‬
‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﺃﻤﺎ‬ ،‫ﻤﺸﻊ‬ ‫ﻏﻴﺭ‬
‫ܪ‬
ଵ
ଷ
‫ﻋﻨﺼﺭ‬ ‫ﻤﻥ‬ ‫ﺍﻨﻁﻼﻗﺎ‬ ‫ﻋﻠﻴﻪ‬ ‫ﺍﻟﺤﺼﻭﻝ‬ ‫ﻴﻤﻜﻥ‬
ܺ
௓
஺
‫ﺍﻟﻤﻌﺎﺩﻟﺔ‬ ‫ﺤﺴﺏ‬ ‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬ ‫ﺒﻌﺩ‬
:‫ﺍﻟﺘﺎﻟﻴﺔ‬
ܺ
௓
஺
൅ ݊
଴
ଵ
՜ ‫݁ܪ‬
ʹ
Ͷ
൅ ‫ܪ‬
ͳ
͵
‫ﺃ‬
-
‫ﺍﻟﻨﻭﺍﺓ‬ ‫ﺭﻤﺯ‬ ‫ﺩ‬
‫ﺩ‬‫ﺤ‬
ܺ
௓
஺
:‫ﺍﻟﺘﺎﻟﻴﺔ‬ ‫ﺍﻷﻨﻭﻴﺔ‬ ‫ﺒﻴﻥ‬ ‫ﻤﻥ‬

ͷ
،
‡
Ͷ
،
‹
͵
،
‡
ʹ
.
‫ﺏ‬
-
‫ﺍﺴﺘﻬﻼﻙ‬ ‫ﻋﻥ‬ ‫ﺍﻟﻨﺎﺘﺠﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﺍﺤﺴﺏ‬
ൌͳ‰
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻤﻥ‬
‫ܪ‬
ଵ
ଶ
.
‫ﺝ‬
-
‫ﺒـ‬ ‫ﺭ‬
‫ﺩ‬‫ﻴﻘ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﻤﻥ‬ ‫ﺍﻟﺴﻨﻭﻱ‬ ‫ﺍﻻﺴﺘﻬﻼﻙ‬


ʹͲ
ൌͶšͳͲ
‫ﺍﻟﻁﺎﻗـﺔ‬ ‫ﻝ‬
‫ﻭ‬‫ﺘﺤـ‬ ‫ﻤﺭﺩﻭﺩ‬ ‫ﺒﺎﻋﺘﺒﺎﺭ‬ ،
‫ﺒـ‬ ‫ﺭ‬
‫ﺩ‬‫ﻴﻘ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺤﺭﺍﺭﻴﺔ‬
͵͵Ψ
.
-
‫ﺍﻟﻌﺎﻟﻤ‬ ‫ﺍﻟﻤﺨﺯﻭﻥ‬ ‫ﻻﺴﺘﻬﻼﻙ‬ ‫ﺍﻟﻼﺯﻤﺔ‬ ‫ﺍﻟﺯﻤﻨﻴﺔ‬ ‫ﺍﻟﻤﺩﺓ‬ ‫ﺒﺎﻟﺴﻨﻭﺍﺕ‬ ‫ﺍﺤﺴﺏ‬
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻤﻥ‬ ‫ﻲ‬
‫ܪ‬
ଵ
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‫ﺍ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﻴﺤﺘﻭﻱ‬
‫ﺍ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﺤﺘﻭﻱ‬
14
(‫ﻨﻘﻁﺔ‬
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‫ﻟﻜﻥ‬ ،‫ﻟﻠﺤﺭﺍﺭﺓ‬ ‫ﻨﺎﺸﺭ‬ ‫ﻋﻝ‬
‫ﻟﻠﺤﺭﺍﺭ‬ ‫ﺸﺭ‬
‫ﻔﻭﻕ‬
ͳͲͲ
ͳͲͲ
‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬
‫ﻭﻥ‬
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺭﻴﻥ‬
‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻥ‬
‫ܪ‬
ଵ
ଶ
‫ﺘﻔﻭﻕ‬ ‫ﻟﻴﺔ‬
‫ﻔﻭﻕ‬
ͳͲͲ
ͳͲͲ
‫ﺩ‬ ‫ﻤﻠﻴﻭﻥ‬
‫ﻤﻠﻴ‬
ଶ
‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬
‫ﻟﺘﺭﻴﺘﻴﻭﻡ‬
‫ܪ‬
‫ܪ‬
ଵ
ଷ
.
.‫ﻋﻝ‬
‫ﺒــ‬ ‫ﻤﻨﻪ‬ ‫ﻲ‬
‫ﺒــ‬ ‫ﻪ‬
‰
‰
ͳ͸
͸
ͳͲ
‫ﺤﺴﺏ‬ ‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬ ‫ﺒﻌﺩ‬
‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬
‫ﻟﻁﺎﻗـﺔ‬
‫ـﺔ‬
3as.ency-education.com
‫ﺻﻔﺤﺔ‬
‫ﻣﻦ‬
10
:‫ﺍﻟﻤﻌﻁﻴﺎﺕ‬
݉ሺ ‫ܪ‬
ଵ
ଷ ሻ ൌ ͵ǡͲͳͷͷ‫ݑ‬
،
݉ሺ ‫ܪ‬
ଵ
ଶ ሻ ൌ ʹǡͲͳ͵ͷͷ‫ݑ‬
،
݉ሺ ‫݁ܪ‬
ଶ
ସ ሻ ൌ ͶǡͲͲͳͷ‫ݑ‬
݉ሺ ݊
଴
ଵ ሻ ൌ ͳǡͲͲͺ͸͸‫ݑ‬
،
ͳ‫ܸ݁ܯ‬ ൌ ͳǡ͸Ͳʹʹ ൈ ͳͲିଵଷ
‫ܬ‬
،
ܰ஺ ൌ ͸ǡͲʹʹ ൈ ͳͲଶଷ
݉‫݈݋‬ିଵ
ͳ‫ݑ‬ ൌ ͻ͵ͳǡͷ‫ܸ݁ܯ‬Ȁܿ;
،
ͳ‫ݑ‬ ൌ ͳǡ͸͸Ͳͷ ൈ ͳͲିଶ଻
‫݃ܭ‬
.
) :‫ﺍﻟﺜﺎﻨﻲ‬ ‫ﺍﻟﺘﻤﺭﻴﻥ‬
06
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‫ﻤﻥ‬ ‫ﺍﻟﻤﻜﺜﻔﺎﺕ‬ ‫ﺘﻌﺘﺒﺭ‬
،‫ﺍﻟﻨﻘﺎﻝ‬ ‫ﺍﻟﻬﺎﺘﻑ‬ ‫ﺸﺎﺤﻥ‬ ‫ﺘﺭﻜﻴﺏ‬ ‫ﻓﻲ‬ ‫ﺘﺩﺨﻝ‬ ‫ﺍﻟﺘﻲ‬ ‫ﺍﻷﺴﺎﺴﻴﺔ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻌﻨﺎﺼﺭ‬
‫ﺍﻟﻤﻘﺎﺒﻠﺔ‬ ‫ﺍﻟﺼﻭﺭﺓ‬ ‫ﺘﻤﺜﻝ‬
‫ﻋﻠﻴﻬﺎ‬ ‫ﻤﺩﻭﻥ‬ ‫ﻭﺍﻀﺤﺔ‬ ‫ﻏﻴﺭ‬ ‫ﺴﻌﺘﻬﺎ‬ ‫ﻨﻘﺎﻝ‬ ‫ﻫﺎﺘﻑ‬ ‫ﺸﺎﺤﻥ‬ ‫ﻤﻥ‬ ‫ﺍﺴﺘﺨﺭﺍﺠﻬﺎ‬ ‫ﺘﻡ‬ ‫ﻤﻜﺜﻔﺔ‬
ሺͶͲͲሻ
.
‫ﺴﻌﺘﻬﺎ‬ ‫ﻤﻌﺭﻓﺔ‬ ‫ﺃﺠﻝ‬ ‫ﻤﻥ‬

‫ﻤﻘﺎﻭﻤﺘـﻪ‬ ‫ﺃﻭﻤﻲ‬ ‫ﻨﺎﻗﻝ‬ ‫ﻤﻊ‬ ‫ﺍﻟﺘﺴﻠﺴﻝ‬ ‫ﻋﻠﻰ‬ ‫ﻨﺭﻜﺒﻬﺎ‬ ‫ﺜﻡ‬ ‫ﻜﻠﻴﺎ‬ ‫ﻨﻔﺭﻏﻬﺎ‬
ܴ ൌ ͳʹǡͷ‫ܭ‬ȳ
‫ﻤﻭﻟـﺩ‬ ،
‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻤﺤﺭﻜﺔ‬ ‫ﻗﻭﺘﻪ‬ ‫ﺜﺎﺒﺕ‬ ‫ﺘﻭﺘﺭ‬
ൌͳʹ
‫ﺒﺎﺩﻟﺔ‬ ،

‫)ﺍﻟﺸﻜﻝ‬ ‫ﻓﻲ‬ ‫ﻤﻭﻀﺢ‬ ‫ﻫﻭ‬ ‫ﻜﻤﺎ‬ .‫ﺘﻭﺼﻴﻝ‬ ‫ﺃﺴﻼﻙ‬ ‫ﻭ‬
-
Ͳͳ
.(
Ǥ
‫ﺍﻟﻠﺤﻅﺔ‬ ‫ﻋﻨﺩ‬
–ൌͲ
) ‫ﺍﻟﻭﻀﻊ‬ ‫ﻓﻲ‬ ‫ﺍﻟﺒﺎﺩﻟﺔ‬ ‫ﻨﻀﻊ‬
ͳ
:(
ͳ
-
.‫ﺍﻟﻜﻬﺭﺒﺎﺌﻲ‬ ‫ﺍﻟﺘﻴﺎﺭ‬ ‫ﺠﻬﺔ‬ ‫ﻭ‬ ‫ﺒﺄﺴﻬﻡ‬ ‫ﺍﻟﺘﻭﺘﺭﺍﺕ‬ ‫ﻋﻠﻴﻬﺎ‬ ‫ﻤﻭﻀﺤﺎ‬ ‫ﺍﻟﺩﺍﺭﺓ‬ ‫ﺭﺴﻡ‬ ‫ﺃﻋﺩ‬
ʹ
-
‫ﻋﻠﻰ‬ ‫ﻥ‬
‫ﻴ‬‫ﺒ‬
‫ﻨﻔﺱ‬
‫ﻟﻤﺸﺎﻫﺩﺓ‬ ‫ﺍﻻﻫﺘﺯﺍﺯ‬ ‫ﺭﺍﺴﻡ‬ ‫ﺭﺒﻁ‬ ‫ﻜﻴﻔﻴﺔ‬ ‫ﺍﻟﺩﺍﺭﺓ‬
‫ﺍﻟﺘﻭﺘﺭ‬
ሺ–ሻ

—
.
͵
-
.‫ﺍﻟﻤﺠﻬﺭﻱ‬ ‫ﺍﻟﻤﺴﺘﻭﻯ‬ ‫ﻋﻠﻰ‬ ‫ﺍﻟﻤﻜﺜﻔﺔ‬ ‫ﺸﺤﻥ‬ ‫ﻴﺘﻡ‬ ‫ﻜﻴﻑ‬ ‫ﻥ‬
‫ﻴ‬‫ﺒ‬
Ͷ
-
‫ﺃﺜﺒ‬
‫ـ‬
‫ﺍﻟﻤﻌ‬ ‫ﺃﻥ‬ ‫ﺕ‬
‫ـ‬
‫ﺍﻟﺘﻔ‬ ‫ﺎﺩﻟﺔ‬
‫ـ‬
‫ﺍﻟﺘ‬ ‫ﺎﻀﻠﻴﺔ‬
‫ـ‬
‫ﻴﺤﻘﻘ‬ ‫ﻲ‬
‫ـ‬
‫ﺍﻟﺘ‬ ‫ﻬﺎ‬
‫ـ‬
‫ﺍﻟﻜﻬﺭﺒﺎﺌﻲ‬ ‫ﻭﺘﺭ‬
ሺ–ሻ

—
:‫ﻫﻲ‬
ௗ௨ೃሺ௧ሻ
ௗ௧
൅
ଵ
ோ஼
‫ݑ‬ோሺ‫ݐ‬ሻ ൌ Ͳ
.
ͷ
-
‫ﺍﻟﺸﻜﻝ‬ ‫ﻤﻥ‬ ‫ﺤﻼ‬ ‫ﺍﻟﺴﺎﺒﻘﺔ‬ ‫ﺍﻟﺘﻔﺎﻀﻠﻴﺔ‬ ‫ﺍﻟﻤﻌﺎﺩﻟﺔ‬ ‫ﺘﻘﺒﻝ‬
‫ݑ‬ோሺ‫ݐ‬ሻ ൌ ‫݁ܣ‬ି
೟
ಳ
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‫ﺃ‬
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‫ﺍﻟﺜﺎﺒﺘﻴﻥ‬ ‫ﻋﺒﺎﺭﺘﻲ‬ ‫ﺩ‬
‫ﺩ‬‫ﺤ‬

‫ﻭ‬

.‫ﺍﻟﺩﺍﺭﺓ‬ ‫ﻤﻤﻴﺯﺍﺕ‬ ‫ﺒﺩﻻﻟﺔ‬
‫ﺏ‬
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‫ﻟﻠﺜﺎﺒﺕ‬ ‫ﺍﻟﻔﻴﺯﻴﺎﺌﻲ‬ ‫ﺍﻟﻤﺩﻟﻭﻝ‬ ‫ﺃﻋﻁ‬

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‫ﺝ‬
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‫ﺃﻥ‬ ‫ﻥ‬
‫ﻴ‬‫ﺒ‬ ،‫ﺍﻟﺒﻌﺩﻱ‬ ‫ﺒﺎﻟﺘﺤﻠﻴﻝ‬

‫ﺜـﻡ‬ ‫ﺍﻟـﺯﻤﻥ‬ ‫ﻤـﻊ‬ ‫ﻤﺘﺠﺎﻨﺱ‬
.‫ﺍﻟﻔﻴﺯﻴﺎﺌﻲ‬ ‫ﻤﺩﻟﻭﻟﻪ‬ ‫ﺍﺴﺘﻨﺘﺞ‬
͸
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‫ﺘﻐﻴـﺭﺍﺕ‬ ‫ﺒﻴـﺎﻥ‬ ‫ﺭﺴـﻡ‬ ‫ﻤـﻥ‬ ‫ﺘﻤﻜﻨﺎ‬ ‫ﻤﻨﺎﺴﺒﺔ‬ ‫ﺒﺭﻤﺠﻴﺔ‬ ‫ﺒﻭﺍﺴﻁﺔ‬
ސ ቀ
஺
௨ೃ
ቁ
‫ﺍﻟﺯﻤﻥ‬ ‫ﺒﺩﻻﻟﺔ‬
–
‫)ﺍﻟﺸﻜﻝ‬ ‫ﻓﻲ‬ ‫ﺢ‬
‫ﻀ‬‫ﻤﻭ‬ ‫ﻫﻭ‬ ‫ﻜﻤﺎ‬
-
Ͳʹ
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:‫ﺍﻟﺒﻴﺎﻥ‬ ‫ﺒﺎﺴﺘﻐﻼﻝ‬
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‫ﺍﻟﺜﺎﺒﺕ‬ ‫ﻗﻴﻤﺔ‬ ‫ﺠﺩ‬

‫ﺍﻟﻤﻜﺜﻔﺔ‬ ‫ﺴﻌﺔ‬ ‫ﻗﻴﻤﺔ‬ ‫ﺍﺴﺘﻨﺘﺞ‬ ‫ﺜﻡ‬

.
Ǥ

Studyadz 3as-physique-c3-59-76

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    ر‬GH8 ‫ن‬J!#‫ا‬ :‫دورة‬ 9 201 :‫ا‬ + ‫ت‬R‫ر‬ ST‫ر‬UV/W XY1Z‫ا‬ ‫ا]م‬ :‫دة‬# 4^ ‫ا_!ر‬ :‫ة‬+`a‫ا‬ 04 c ‫و‬ 30 ‫د‬ :‫ﺍﻟﺘﺎﻟﻴﻴﻥ‬ ‫ﺍﻟﻤﻭﻀﻭﻋﻴﻥ‬ ‫ﺃﺤﺩ‬ ‫ﻴﺨﺘﺎﺭ‬ ‫ﺃﻥ‬ ‫ﺍﻟﻤﺘﺭﺸﺢ‬ ‫ﻋﻠﻰ‬ ‫ﺍﻷﻭﻝ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﻋﻠﻰ‬ ‫ﺍﻷﻭﻝ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﻴﺤﺘﻭﻱ‬ 05 ‫ﺍﻟﺼﻔﺤﺔ‬ ‫ﻤﻥ‬ ) ‫ﺼﻔﺤﺎﺕ‬ 1 ‫ﻤﻥ‬ 10 ‫ﺍﻟﺼﻔﺤﺔ‬ ‫ﺇﻟﻰ‬ 5 ‫ﻤﻥ‬ 10 ( ) :‫ﺍﻷﻭﻝ‬ ‫ﺍﻟﺠﺯء‬ 14 (‫ﻨﻘﻁﺔ‬ ):‫ﺍﻷﻭﻝ‬ ‫ﺍﻟﺘﻤﺭﻴﻥ‬ 04 (‫ﻥ‬ ‫ﺍﻻﻨﺩﻤﺎﺝ‬ ‫ﺘﻔﺎﻋﻝ‬ ‫ﺘﺴـﺨﻴﻥ‬ ‫ﻀـﺭﻭﺭﺓ‬ :‫ﺒﻴﻨﻬﺎ‬ ‫ﻤﻥ‬ ‫ﺘﻘﻨﻴﺔ‬ ‫ﺼﻌﻭﺒﺎﺕ‬ ‫ﻋﺩﺓ‬ ‫ﻴﻁﺭﺡ‬ ‫ﺇﻨﺠﺎﺯﻩ‬ ‫ﻟﻜﻥ‬ ،‫ﻟﻠﺤﺭﺍﺭﺓ‬ ‫ﻨﺎﺸﺭ‬ ‫ﺘﻔﺎﻋﻝ‬ ‫ﺍﻟﻨﻭﻭﻱ‬ ‫ﺘﻔﻭﻕ‬ ‫ﻋﺎﻟﻴﺔ‬ ‫ﺤﺭﺍﺭﺓ‬ ‫ﺩﺭﺠﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺨﻠﻴﻁ‬ ͳͲͲ .‫ﺍﻟﺘﻔﺎﻋﻝ‬ ‫ﺍﻨﻁﻼﻕ‬ ‫ﻟﻀﻤﺎﻥ‬ ‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬ ‫ﻤ‬ ‫ﺒ‬ ‫ﻥ‬ ‫ﻴ‬ ‫ﺍﻻﻨﺩﻤ‬ ‫ﺘﻔﺎﻋﻼﺕ‬ ‫ﻥ‬ ‫ـ‬ ‫ﺎﺝ‬ ، ‫ﺍﻟﻨﻅﻴ‬ ‫ﺍﻨﺩﻤﺎﺝ‬ ‫ـ‬ ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺭﻴﻥ‬ ‫ܪ‬ ଵ ଶ ‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬ ‫ܪ‬ ଵ ଷ ‫ﺍﻟﻬﻴﻠﻴ‬ ‫ﻨﻭﺍﺓ‬ ‫ﻴﻌﻁﻲ‬ ‫ﺍﻟﺫﻱ‬ ‫ﻭ‬ ‫ـ‬ ‫ﻭﻡ‬ ‫݁ܪ‬ ଶ ସ ‫ﻨﺘﺭﻭﻥ‬ ‫ﻭ‬ ݊ ଴ ଵ . ͳ - .‫ﺍﻟﻨﻅﺎﺌﺭ‬ ،‫ﺍﻟﻨﻭﻭﻱ‬ ‫ﺍﻻﻨﺩﻤﺎﺝ‬ :‫ﻴﻠﻲ‬ ‫ﻤﺎ‬ ‫ﻑ‬ ‫ﺭ‬‫ﻋ‬ ʹ - ‫ﺘﻔﻭﻕ‬ ‫ﻋﺎﻟﻴﺔ‬ ‫ﺤﺭﺍﺭﺓ‬ ‫ﺩﺭﺠﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺨﻠﻴﻁ‬ ‫ﺘﺴﺨﻴﻥ‬ ‫ﻴﺘﻡ‬ ‫ﻟﻤﺎﺫﺍ‬ ‫ﺍﺸﺭﺡ‬ ͳͲͲ .‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬ ͵ - ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺍﻟﻨﻅﻴﺭﻴﻥ‬ ‫ﺒﻴﻥ‬ ‫ﺍﻟﻨﻭﻭﻱ‬ ‫ﺍﻻﻨﺩﻤﺎﺝ‬ ‫ﻤﻌﺎﺩﻟﺔ‬ ‫ﺍﻜﺘﺏ‬ ‫ܪ‬ ଵ ଶ ‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬ ‫ܪ‬ ଵ ଷ . Ͷ - ‫ﺒﺎﻟـ‬ ‫ﺍﺤﺴﺏ‬ ‡ ‫ﺒﺎﻟـ‬ ‫ﺜﻡ‬ ‘—Ž .‫ﺍﻟﺘﻔﺎﻋﻝ‬ ‫ﻫﺫﺍ‬ ‫ﺭﻫﺎ‬ ‫ﺭ‬‫ﻴﺤ‬ ‫ﺍﻟﺘﻲ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ͷ - ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻴﻭﺠﺩ‬ ‫ܪ‬ ଵ ଶ ‫ﺒــ‬ ‫ﻤﻨﻪ‬ ‫ﺍﻟﻌﺎﻟﻤﻲ‬ ‫ﺍﻻﺤﺘﻴﺎﻁ‬ ‫ﺭ‬ ‫ﺩ‬‫ﻴﻘ‬ ‫ﺤﻴﺙ‬ ،‫ﺍﻟﻤﺤﻴﻁﺎﺕ‬ ‫ﻓﻲ‬ ‫ﺒﻭﻓﺭﺓ‬ ‰ ͳ͸ Ͷǡ͸šͳͲ ‫ﻫـﻭ‬ ‫ﻭ‬ ‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﺃﻤﺎ‬ ،‫ﻤﺸﻊ‬ ‫ﻏﻴﺭ‬ ‫ܪ‬ ଵ ଷ ‫ﻋﻨﺼﺭ‬ ‫ﻤﻥ‬ ‫ﺍﻨﻁﻼﻗﺎ‬ ‫ﻋﻠﻴﻪ‬ ‫ﺍﻟﺤﺼﻭﻝ‬ ‫ﻴﻤﻜﻥ‬ ܺ ௓ ஺ ‫ﺍﻟﻤﻌﺎﺩﻟﺔ‬ ‫ﺤﺴﺏ‬ ‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬ ‫ﺒﻌﺩ‬ :‫ﺍﻟﺘﺎﻟﻴﺔ‬ ܺ ௓ ஺ ൅ ݊ ଴ ଵ ՜ ‫݁ܪ‬ ʹ Ͷ ൅ ‫ܪ‬ ͳ ͵ ‫ﺃ‬ - ‫ﺍﻟﻨﻭﺍﺓ‬ ‫ﺭﻤﺯ‬ ‫ﺩ‬ ‫ﺩ‬‫ﺤ‬ ܺ ௓ ஺ :‫ﺍﻟﺘﺎﻟﻴﺔ‬ ‫ﺍﻷﻨﻭﻴﺔ‬ ‫ﺒﻴﻥ‬ ‫ﻤﻥ‬ ͷ ، ‡ Ͷ ، ‹ ͵ ، ‡ ʹ . ‫ﺏ‬ - ‫ﺍﺴﺘﻬﻼﻙ‬ ‫ﻋﻥ‬ ‫ﺍﻟﻨﺎﺘﺠﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﺍﺤﺴﺏ‬ ൌͳ‰ ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻤﻥ‬ ‫ܪ‬ ଵ ଶ . ‫ﺝ‬ - ‫ﺒـ‬ ‫ﺭ‬ ‫ﺩ‬‫ﻴﻘ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﻤﻥ‬ ‫ﺍﻟﺴﻨﻭﻱ‬ ‫ﺍﻻﺴﺘﻬﻼﻙ‬ ʹͲ ൌͶšͳͲ ‫ﺍﻟﻁﺎﻗـﺔ‬ ‫ﻝ‬ ‫ﻭ‬‫ﺘﺤـ‬ ‫ﻤﺭﺩﻭﺩ‬ ‫ﺒﺎﻋﺘﺒﺎﺭ‬ ، ‫ﺒـ‬ ‫ﺭ‬ ‫ﺩ‬‫ﻴﻘ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻁﺎﻗﺔ‬ ‫ﺇﻟﻰ‬ ‫ﺍﻟﺤﺭﺍﺭﻴﺔ‬ ͵͵Ψ . - ‫ﺍﻟﻌﺎﻟﻤ‬ ‫ﺍﻟﻤﺨﺯﻭﻥ‬ ‫ﻻﺴﺘﻬﻼﻙ‬ ‫ﺍﻟﻼﺯﻤﺔ‬ ‫ﺍﻟﺯﻤﻨﻴﺔ‬ ‫ﺍﻟﻤﺩﺓ‬ ‫ﺒﺎﻟﺴﻨﻭﺍﺕ‬ ‫ﺍﺤﺴﺏ‬ ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻤﻥ‬ ‫ﻲ‬ ‫ܪ‬ ଵ ଶ Ǥ B e n c y - e d u c a t i o n . c o m / e x a m s ‫ا‬ 4^ ‫ا_!ر‬ !_‫ا‬ s m s ‫ﺍ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﻴﺤﺘﻭﻱ‬ ‫ﺍ‬ ‫ﺍﻟﻤﻭﻀﻭﻉ‬ ‫ﺤﺘﻭﻱ‬ 14 (‫ﻨﻘﻁﺔ‬ (‫ﻨﻘﻁﺔ‬ (‫ﻥ‬ ‫ﻟﻜﻥ‬ ،‫ﻟﻠﺤﺭﺍﺭﺓ‬ ‫ﻨﺎﺸﺭ‬ ‫ﻋﻝ‬ ‫ﻟﻠﺤﺭﺍﺭ‬ ‫ﺸﺭ‬ ‫ﻔﻭﻕ‬ ͳͲͲ ͳͲͲ ‫ﺩﺭﺠﺔ‬ ‫ﻤﻠﻴﻭﻥ‬ ‫ﻭﻥ‬ ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﺭﻴﻥ‬ ‫ﺍﻟﺩﻴﺘﻴﺭﻴﻭﻡ‬ ‫ﻥ‬ ‫ܪ‬ ଵ ଶ ‫ﺘﻔﻭﻕ‬ ‫ﻟﻴﺔ‬ ‫ﻔﻭﻕ‬ ͳͲͲ ͳͲͲ ‫ﺩ‬ ‫ﻤﻠﻴﻭﻥ‬ ‫ﻤﻠﻴ‬ ଶ ‫ﺍﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ﻭ‬ ‫ﻟﺘﺭﻴﺘﻴﻭﻡ‬ ‫ܪ‬ ‫ܪ‬ ଵ ଷ . .‫ﻋﻝ‬ ‫ﺒــ‬ ‫ﻤﻨﻪ‬ ‫ﻲ‬ ‫ﺒــ‬ ‫ﻪ‬ ‰ ‰ ͳ͸ ͸ ͳͲ ‫ﺤﺴﺏ‬ ‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬ ‫ﺒﻌﺩ‬ ‫ﺒﻨﺘﺭﻭﻥ‬ ‫ﻗﺫﻓﻪ‬ ‫ﻟﻁﺎﻗـﺔ‬ ‫ـﺔ‬ 3as.ency-education.com
  • 9.
    ‫ﺻﻔﺤﺔ‬ ‫ﻣﻦ‬ 10 :‫ﺍﻟﻤﻌﻁﻴﺎﺕ‬ ݉ሺ ‫ܪ‬ ଵ ଷ ሻൌ ͵ǡͲͳͷͷ‫ݑ‬ ، ݉ሺ ‫ܪ‬ ଵ ଶ ሻ ൌ ʹǡͲͳ͵ͷͷ‫ݑ‬ ، ݉ሺ ‫݁ܪ‬ ଶ ସ ሻ ൌ ͶǡͲͲͳͷ‫ݑ‬ ݉ሺ ݊ ଴ ଵ ሻ ൌ ͳǡͲͲͺ͸͸‫ݑ‬ ، ͳ‫ܸ݁ܯ‬ ൌ ͳǡ͸Ͳʹʹ ൈ ͳͲିଵଷ ‫ܬ‬ ، ܰ஺ ൌ ͸ǡͲʹʹ ൈ ͳͲଶଷ ݉‫݈݋‬ିଵ ͳ‫ݑ‬ ൌ ͻ͵ͳǡͷ‫ܸ݁ܯ‬Ȁܿ; ، ͳ‫ݑ‬ ൌ ͳǡ͸͸Ͳͷ ൈ ͳͲିଶ଻ ‫݃ܭ‬ . ) :‫ﺍﻟﺜﺎﻨﻲ‬ ‫ﺍﻟﺘﻤﺭﻴﻥ‬ 06 (‫ﻥ‬ ‫ﻤﻥ‬ ‫ﺍﻟﻤﻜﺜﻔﺎﺕ‬ ‫ﺘﻌﺘﺒﺭ‬ ،‫ﺍﻟﻨﻘﺎﻝ‬ ‫ﺍﻟﻬﺎﺘﻑ‬ ‫ﺸﺎﺤﻥ‬ ‫ﺘﺭﻜﻴﺏ‬ ‫ﻓﻲ‬ ‫ﺘﺩﺨﻝ‬ ‫ﺍﻟﺘﻲ‬ ‫ﺍﻷﺴﺎﺴﻴﺔ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻌﻨﺎﺼﺭ‬ ‫ﺍﻟﻤﻘﺎﺒﻠﺔ‬ ‫ﺍﻟﺼﻭﺭﺓ‬ ‫ﺘﻤﺜﻝ‬ ‫ﻋﻠﻴﻬﺎ‬ ‫ﻤﺩﻭﻥ‬ ‫ﻭﺍﻀﺤﺔ‬ ‫ﻏﻴﺭ‬ ‫ﺴﻌﺘﻬﺎ‬ ‫ﻨﻘﺎﻝ‬ ‫ﻫﺎﺘﻑ‬ ‫ﺸﺎﺤﻥ‬ ‫ﻤﻥ‬ ‫ﺍﺴﺘﺨﺭﺍﺠﻬﺎ‬ ‫ﺘﻡ‬ ‫ﻤﻜﺜﻔﺔ‬ ሺͶͲͲሻ . ‫ﺴﻌﺘﻬﺎ‬ ‫ﻤﻌﺭﻓﺔ‬ ‫ﺃﺠﻝ‬ ‫ﻤﻥ‬ ‫ﻤﻘﺎﻭﻤﺘـﻪ‬ ‫ﺃﻭﻤﻲ‬ ‫ﻨﺎﻗﻝ‬ ‫ﻤﻊ‬ ‫ﺍﻟﺘﺴﻠﺴﻝ‬ ‫ﻋﻠﻰ‬ ‫ﻨﺭﻜﺒﻬﺎ‬ ‫ﺜﻡ‬ ‫ﻜﻠﻴﺎ‬ ‫ﻨﻔﺭﻏﻬﺎ‬ ܴ ൌ ͳʹǡͷ‫ܭ‬ȳ ‫ﻤﻭﻟـﺩ‬ ، ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻴﺔ‬ ‫ﺍﻟﻤﺤﺭﻜﺔ‬ ‫ﻗﻭﺘﻪ‬ ‫ﺜﺎﺒﺕ‬ ‫ﺘﻭﺘﺭ‬ ൌͳʹ ‫ﺒﺎﺩﻟﺔ‬ ، ‫)ﺍﻟﺸﻜﻝ‬ ‫ﻓﻲ‬ ‫ﻤﻭﻀﺢ‬ ‫ﻫﻭ‬ ‫ﻜﻤﺎ‬ .‫ﺘﻭﺼﻴﻝ‬ ‫ﺃﺴﻼﻙ‬ ‫ﻭ‬ - Ͳͳ .( Ǥ
  • 10.
    ‫ﺍﻟﻠﺤﻅﺔ‬ ‫ﻋﻨﺩ‬ –ൌͲ ) ‫ﺍﻟﻭﻀﻊ‬‫ﻓﻲ‬ ‫ﺍﻟﺒﺎﺩﻟﺔ‬ ‫ﻨﻀﻊ‬ ͳ :( ͳ - .‫ﺍﻟﻜﻬﺭﺒﺎﺌﻲ‬ ‫ﺍﻟﺘﻴﺎﺭ‬ ‫ﺠﻬﺔ‬ ‫ﻭ‬ ‫ﺒﺄﺴﻬﻡ‬ ‫ﺍﻟﺘﻭﺘﺭﺍﺕ‬ ‫ﻋﻠﻴﻬﺎ‬ ‫ﻤﻭﻀﺤﺎ‬ ‫ﺍﻟﺩﺍﺭﺓ‬ ‫ﺭﺴﻡ‬ ‫ﺃﻋﺩ‬ ʹ - ‫ﻋﻠﻰ‬ ‫ﻥ‬ ‫ﻴ‬‫ﺒ‬ ‫ﻨﻔﺱ‬ ‫ﻟﻤﺸﺎﻫﺩﺓ‬ ‫ﺍﻻﻫﺘﺯﺍﺯ‬ ‫ﺭﺍﺴﻡ‬ ‫ﺭﺒﻁ‬ ‫ﻜﻴﻔﻴﺔ‬ ‫ﺍﻟﺩﺍﺭﺓ‬ ‫ﺍﻟﺘﻭﺘﺭ‬ ሺ–ሻ — . ͵ - .‫ﺍﻟﻤﺠﻬﺭﻱ‬ ‫ﺍﻟﻤﺴﺘﻭﻯ‬ ‫ﻋﻠﻰ‬ ‫ﺍﻟﻤﻜﺜﻔﺔ‬ ‫ﺸﺤﻥ‬ ‫ﻴﺘﻡ‬ ‫ﻜﻴﻑ‬ ‫ﻥ‬ ‫ﻴ‬‫ﺒ‬ Ͷ - ‫ﺃﺜﺒ‬ ‫ـ‬ ‫ﺍﻟﻤﻌ‬ ‫ﺃﻥ‬ ‫ﺕ‬ ‫ـ‬ ‫ﺍﻟﺘﻔ‬ ‫ﺎﺩﻟﺔ‬ ‫ـ‬ ‫ﺍﻟﺘ‬ ‫ﺎﻀﻠﻴﺔ‬ ‫ـ‬ ‫ﻴﺤﻘﻘ‬ ‫ﻲ‬ ‫ـ‬ ‫ﺍﻟﺘ‬ ‫ﻬﺎ‬ ‫ـ‬ ‫ﺍﻟﻜﻬﺭﺒﺎﺌﻲ‬ ‫ﻭﺘﺭ‬ ሺ–ሻ — :‫ﻫﻲ‬ ௗ௨ೃሺ௧ሻ ௗ௧ ൅ ଵ ோ஼ ‫ݑ‬ோሺ‫ݐ‬ሻ ൌ Ͳ . ͷ - ‫ﺍﻟﺸﻜﻝ‬ ‫ﻤﻥ‬ ‫ﺤﻼ‬ ‫ﺍﻟﺴﺎﺒﻘﺔ‬ ‫ﺍﻟﺘﻔﺎﻀﻠﻴﺔ‬ ‫ﺍﻟﻤﻌﺎﺩﻟﺔ‬ ‫ﺘﻘﺒﻝ‬ ‫ݑ‬ோሺ‫ݐ‬ሻ ൌ ‫݁ܣ‬ି ೟ ಳ . ‫ﺃ‬ - ‫ﺍﻟﺜﺎﺒﺘﻴﻥ‬ ‫ﻋﺒﺎﺭﺘﻲ‬ ‫ﺩ‬ ‫ﺩ‬‫ﺤ‬ ‫ﻭ‬ .‫ﺍﻟﺩﺍﺭﺓ‬ ‫ﻤﻤﻴﺯﺍﺕ‬ ‫ﺒﺩﻻﻟﺔ‬ ‫ﺏ‬ - ‫ﻟﻠﺜﺎﺒﺕ‬ ‫ﺍﻟﻔﻴﺯﻴﺎﺌﻲ‬ ‫ﺍﻟﻤﺩﻟﻭﻝ‬ ‫ﺃﻋﻁ‬ . ‫ﺝ‬ - ‫ﺃﻥ‬ ‫ﻥ‬ ‫ﻴ‬‫ﺒ‬ ،‫ﺍﻟﺒﻌﺩﻱ‬ ‫ﺒﺎﻟﺘﺤﻠﻴﻝ‬ ‫ﺜـﻡ‬ ‫ﺍﻟـﺯﻤﻥ‬ ‫ﻤـﻊ‬ ‫ﻤﺘﺠﺎﻨﺱ‬ .‫ﺍﻟﻔﻴﺯﻴﺎﺌﻲ‬ ‫ﻤﺩﻟﻭﻟﻪ‬ ‫ﺍﺴﺘﻨﺘﺞ‬ ͸ - ‫ﺘﻐﻴـﺭﺍﺕ‬ ‫ﺒﻴـﺎﻥ‬ ‫ﺭﺴـﻡ‬ ‫ﻤـﻥ‬ ‫ﺘﻤﻜﻨﺎ‬ ‫ﻤﻨﺎﺴﺒﺔ‬ ‫ﺒﺭﻤﺠﻴﺔ‬ ‫ﺒﻭﺍﺴﻁﺔ‬ ސ ቀ ஺ ௨ೃ ቁ ‫ﺍﻟﺯﻤﻥ‬ ‫ﺒﺩﻻﻟﺔ‬ – ‫)ﺍﻟﺸﻜﻝ‬ ‫ﻓﻲ‬ ‫ﺢ‬ ‫ﻀ‬‫ﻤﻭ‬ ‫ﻫﻭ‬ ‫ﻜﻤﺎ‬ - Ͳʹ .( :‫ﺍﻟﺒﻴﺎﻥ‬ ‫ﺒﺎﺴﺘﻐﻼﻝ‬ - ‫ﺍﻟﺜﺎﺒﺕ‬ ‫ﻗﻴﻤﺔ‬ ‫ﺠﺩ‬ ‫ﺍﻟﻤﻜﺜﻔﺔ‬ ‫ﺴﻌﺔ‬ ‫ﻗﻴﻤﺔ‬ ‫ﺍﺴﺘﻨﺘﺞ‬ ‫ﺜﻡ‬ . Ǥ