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Fourth Year Composite materials
Report: Solution to Homework III
Report No: 3 Date: 18/3/2013
Submitted to: Dr. Mohammad Tawfik
Name
๏‚ท Mohammad Tawfik Eraky
โ€ซุนุฑุงู‚ูŠโ€ฌ โ€ซุฃุญู…ุฏโ€ฌ โ€ซุชูˆููŠู‚โ€ฌ โ€ซู…ุญู…ุฏโ€ฌ
2013/2014
Pb
Given ๐œถ ๐’‡ , ๐œถ ๐’Ž for composite materials calculate ๐œถ ๐Ÿ , ๐œถ ๐Ÿ
Solution
# Main assumptions:
1. ๐ ๐Ÿ = ๐ ๐’‡ = ๐ ๐’Ž
2. ๐ˆ ๐Ÿ = ๐ˆ ๐’‡ = ๐ˆ ๐’Ž
Assuming that interaction force to be =R
And assuming that fibers feels tension, then the total displacement of the fiber should be equal to that
of the matrix so
๐›ผ ๐น ๐ฟ ๐‘“ ๐‘‡ โˆ’
๐‘…๐ฟ ๐น
๐ธ ๐น ๐ด ๐น
โˆ’
๐‘…๐ฟ ๐‘€
๐ธ ๐‘€ ๐ด ๐‘€
โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡ = 0
๐‘… =
๐›ผ ๐น ๐ฟ ๐‘“ โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡
๐ฟ ๐‘“
๐ธ ๐น ๐ด ๐น
+
๐ฟ ๐‘€
๐ธ ๐‘€ ๐ด ๐‘€
ฮ”๐ฟ =
๐ฟ ๐‘€
๐ธ ๐‘€ ๐ด ๐‘€
๐›ผ ๐น ๐ฟ ๐‘“ โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡
๐ฟ ๐‘“
๐ธ ๐น ๐ด ๐น
+
๐ฟ ๐‘€
๐ธ ๐‘€ ๐ด ๐‘€
+ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡
Applying the first assumption
๐ ๐Ÿ =
ฮ”๐ฟ
๐ฟ
=
๐‘‡(
๐›ผ ๐น
๐ธ ๐‘€ ๐ด ๐‘€
+
๐›ผ ๐‘€
๐ธ ๐น ๐ด ๐น
)
1
๐ธ ๐‘€ ๐ด ๐‘€
+
1
๐ธ ๐น ๐ด ๐น
= ๐›ผ1 ๐‘‡
Where
๐œ ๐‘€ =
๐ด
๐ด ๐‘€
, ๐œ ๐น =
๐ด
๐ด ๐น
Then
๐›ผ1 =
๐œ ๐น ๐ธ ๐น ๐›ผ ๐น + ๐œ ๐‘€ ๐ธ ๐‘€ ๐›ผ ๐‘€
๐œ ๐น ๐ธ ๐น + ๐œ ๐‘€ ๐ธ ๐‘€
๐›ฅ๐ฟ = ๐›ฅ๐ฟ ๐น + ๐›ฅ๐ฟ ๐‘€ = ๐›ผ ๐น ๐ฟ ๐‘“2 + ๐›ผ ๐‘€ ๐ฟ ๐‘€2 ๐‘‡
Where subscript 2 refers to the length in the transverse direction normal to fibers and tangent to fiber
matrix plane
๐ ๐Ÿ =
๐›ฅ๐ฟ ๐‘€+๐›ฅ๐ฟ ๐น
๐ฟ ๐‘“ + ๐ฟ ๐‘€
=
๐›ผ ๐น ๐ฟ ๐‘“2 + ๐›ผ ๐‘€ ๐ฟ ๐‘€2 ๐‘‡
๐ฟ ๐‘“ + ๐ฟ ๐‘€
= ๐›ผ2 ๐‘‡
๐›ผ2 = ๐›ผ ๐น ๐‘‰ ๐น + ๐›ผ ๐‘€ ๐‘‰ ๐‘€

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Hw3

  • 1. Fourth Year Composite materials Report: Solution to Homework III Report No: 3 Date: 18/3/2013 Submitted to: Dr. Mohammad Tawfik Name ๏‚ท Mohammad Tawfik Eraky โ€ซุนุฑุงู‚ูŠโ€ฌ โ€ซุฃุญู…ุฏโ€ฌ โ€ซุชูˆููŠู‚โ€ฌ โ€ซู…ุญู…ุฏโ€ฌ 2013/2014
  • 2. Pb Given ๐œถ ๐’‡ , ๐œถ ๐’Ž for composite materials calculate ๐œถ ๐Ÿ , ๐œถ ๐Ÿ Solution # Main assumptions: 1. ๐ ๐Ÿ = ๐ ๐’‡ = ๐ ๐’Ž 2. ๐ˆ ๐Ÿ = ๐ˆ ๐’‡ = ๐ˆ ๐’Ž Assuming that interaction force to be =R And assuming that fibers feels tension, then the total displacement of the fiber should be equal to that of the matrix so ๐›ผ ๐น ๐ฟ ๐‘“ ๐‘‡ โˆ’ ๐‘…๐ฟ ๐น ๐ธ ๐น ๐ด ๐น โˆ’ ๐‘…๐ฟ ๐‘€ ๐ธ ๐‘€ ๐ด ๐‘€ โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡ = 0 ๐‘… = ๐›ผ ๐น ๐ฟ ๐‘“ โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡ ๐ฟ ๐‘“ ๐ธ ๐น ๐ด ๐น + ๐ฟ ๐‘€ ๐ธ ๐‘€ ๐ด ๐‘€ ฮ”๐ฟ = ๐ฟ ๐‘€ ๐ธ ๐‘€ ๐ด ๐‘€ ๐›ผ ๐น ๐ฟ ๐‘“ โˆ’ ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡ ๐ฟ ๐‘“ ๐ธ ๐น ๐ด ๐น + ๐ฟ ๐‘€ ๐ธ ๐‘€ ๐ด ๐‘€ + ๐›ผ ๐‘€ ๐ฟ ๐‘€ ๐‘‡ Applying the first assumption ๐ ๐Ÿ = ฮ”๐ฟ ๐ฟ = ๐‘‡( ๐›ผ ๐น ๐ธ ๐‘€ ๐ด ๐‘€ + ๐›ผ ๐‘€ ๐ธ ๐น ๐ด ๐น ) 1 ๐ธ ๐‘€ ๐ด ๐‘€ + 1 ๐ธ ๐น ๐ด ๐น = ๐›ผ1 ๐‘‡ Where ๐œ ๐‘€ = ๐ด ๐ด ๐‘€ , ๐œ ๐น = ๐ด ๐ด ๐น Then
  • 3. ๐›ผ1 = ๐œ ๐น ๐ธ ๐น ๐›ผ ๐น + ๐œ ๐‘€ ๐ธ ๐‘€ ๐›ผ ๐‘€ ๐œ ๐น ๐ธ ๐น + ๐œ ๐‘€ ๐ธ ๐‘€ ๐›ฅ๐ฟ = ๐›ฅ๐ฟ ๐น + ๐›ฅ๐ฟ ๐‘€ = ๐›ผ ๐น ๐ฟ ๐‘“2 + ๐›ผ ๐‘€ ๐ฟ ๐‘€2 ๐‘‡ Where subscript 2 refers to the length in the transverse direction normal to fibers and tangent to fiber matrix plane ๐ ๐Ÿ = ๐›ฅ๐ฟ ๐‘€+๐›ฅ๐ฟ ๐น ๐ฟ ๐‘“ + ๐ฟ ๐‘€ = ๐›ผ ๐น ๐ฟ ๐‘“2 + ๐›ผ ๐‘€ ๐ฟ ๐‘€2 ๐‘‡ ๐ฟ ๐‘“ + ๐ฟ ๐‘€ = ๐›ผ2 ๐‘‡ ๐›ผ2 = ๐›ผ ๐น ๐‘‰ ๐น + ๐›ผ ๐‘€ ๐‘‰ ๐‘€