3/26/2012 “An Aggie does not lie, cheat, or steal or tolerate those who do” Name Signature EXAM 2 Materials (70 minutes) 1. Determine the ASTM grain size number for the material in the figure with magnification 10,000. ~116 ππππππ ≈ 8.59 ππππππ /ππ2 3ππ × 4.5ππ 8.59 2 ππππππ π−1 10000⁄ × ( ) 100 = 2 ππ2 log(85900) = (π − 1)log(2) n ~17 Page 1 of 8 3/26/2012 “An Aggie does not lie, cheat, or steal or tolerate those who do” 2. What type(s) of bonds are found between atoms within hydrocarbon molecules? (A) ionic bonds (B) covalent bonds (C) van der Waals bonds (D) metallic bonds Page 2 of 8 “An Aggie does not lie, cheat, or steal or tolerate those who do” 3/26/2012 3. Assume there is one Schottky defect in every eight unit cells of ZnS, which has the zinc blende structure, with lattice parameter is 0.59583 nm. What is the density of the defective ceramic? The density of the ceramic In 8 unit cells, we expect 32 Zn + 32 S , but due to the defect: 32 Zn − 1= 31 32 S − 1= 31 π= (31/32)(4)(65.41 π/πππ) + (31/32)(4)(32.06 π/πππ) = 2.97 π/ππ3 ππ‘πππ (5.9583 ∗ 10− 8 ππ)3 (6.02 ∗ 1023 πππ ) ππππ ππ‘π¦ = ππππππ‘ππ£π πππππ πππ π π£πππ’ππ ππ πππππ Page 3 of 8 “An Aggie does not lie, cheat, or steal or tolerate those who do” 3/26/2012 4. Show that C x = ο¦ x2 οΆ οΆC οΆ 2C B ο·ο· is a solution to = D 2 The parameter B is independent exp ο§ο§ ο οΆt οΆx . Dt ο¨ 4Dt οΈ of both x and t. Calculating ο¦ x2 οΆ ο¦ x2 οΆ οΆC B ο§ ο· ο·ο· = ο1 exp ο§ο§ ο οΆt 2D1/ 2t 3 / 2 ο§ο¨ 2Dt ο·οΈ 4 Dt ο¨ οΈ And D οΆ 2C B = 2 1/ 2 3 / 2 οΆx 2D t ο¦ x2 οΆ ο¦ x2 οΆ ο§ο§ ο·ο· ο1 ο·ο·exp ο§ο§ ο 2 Dt 4 Dt ο¨ οΈ ο¨ οΈ Both yield the same results Page 4 of 8 “An Aggie does not lie, cheat, or steal or tolerate those who do” 3/26/2012 5. Iron containing 0.05% C is heated to 912oC in an atmosphere that produces 1.20% C at the surface and is held for 24 h. Calculate the ratio of carbon content (CxBCC/CxFCC) at 0.05 cm beneath the surface. Where CxBCC is the Cx when iron is in a BCC phase and CxFCC for iron in a FCC phase. T= (24 h)(3600 s/h) = 86,400 s π·π΅πΆπΆ = 6.2 × 10 π·πΉπΆπΆ = 2.3 × 10 π΅πΆπΆ: −7 −5 π 2⁄ −80000 π exp ( 8.314 π 1.2 − πΆπ₯ = erf 1.2 − 0.05 2⁄ π½ πππ ) = 1.845 × 10−10 π2 /π π½ πππ ) = 6.883 × 10−12 π2 /π π½ × 1185 πΎ πππ πΎ −148000 π exp ( 8.314 π½ × 1185 πΎ πππ πΎ 0.0005 π √ [2 1.845 × 10−10 π2 × 86,400 π ] π = erf[0.0626] = 0.0705 CxBCC : 1.12% πΉπΆπΆ: 1.2 − πΆπ₯ = erf 1.2 − 0.05 0.0005 π 2 −12 π × 86,400 π √ [2 6.883 × 10 ] π = erf[0.3242] = 0.3532 CxFCC : 0.79% CxBCC/CxFCC = 1.41 Page 5 of 8 3/26/2012 “An Aggie does not lie, cheat, or steal or tolerate those who do” 6. Calculate the molecular weight of a 5000-mers copolymer produced by 1 kg of ethylene and 3 kg of propylene. Page 6 of 8 “An Aggie does not lie, cheat, or steal or tolerate those who do” 3/26/2012 7. The following data (plotted) were collected from a 20 mm diameter test specimen of a ductile cast iron (l0 = 40.00 mm); after fracture, the gage length is 47.42 mm and the diameter is 18.35 mm. Solution Calculate (a) the 0.2% offset yield strength, (b) the tensile strength, (c) the modulus of elasticity, (d) the %Elongation, (e) the %Reduction in area, (f) the engineering stress at fracture, (g) the true stress at fracture (h) the modulus of resilience. ½(yield strength)2(modulus of elasticity)= ½ (240MPa)2(172000MPa) = 0.17 MPa Page 7 of 8 “An Aggie does not lie, cheat, or steal or tolerate those who do” 3/26/2012 8. The net bonding energy EN between two isolated positive and negative ions is a function of A B interionic distance r as follows: E N ο½ ο m ο« n , where A, B, m, and n are constants for the r r particular ion pair. This equation is also valid for the bonding energy between adjacent ions in solid materials. The modulus of elasticity E at the equilibrium interionic separation ro is, ο¦ dF οΆ E ο½ Lο§ ο· ο¨ dr οΈ ro . Derive an expression for the dependence of the modulus of elasticity on these A, B, m, and n parameters (for the two-ion system). πΉ= ππΈπ ππ ππΈπ = π΄ππ0 −(π+1) − π΅ππ0 −(π+1) ππ ππΈπ =0 ππ 1 π¦πππππ → π΄π π−π π0 = ( ) π΅π Solution −(π+2) π−π π΄π ο¦ dF οΆ πΈ = πΏο§ ) ο· = L (−π΄π(π + 1) ( π΅π ο¨ dr οΈ ro −(π+2) π−π π΄π + π΅π(π + 1) ( ) π΅π ) Page 8 of 8