A concrete cylinder having a a diameter of of in. mm and elasticity. Stress and Strain: Stress and Strain: 0.

Size: px
Start display at page:

Download "A concrete cylinder having a a diameter of of in. mm and elasticity. Stress and Strain: Stress and Strain: 0."

Transcription

1 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently concrete cylinder having a a diameter of of in. mm and and gauge gauge length length of 12 of in. 300 is tested mm is in tested compression.the in compression. results The of results the test of are the reported test are in reported the table in as the load table versus as contraction. load versus contraction. Draw the stress strain Draw the diagram stress-strain using scales diagram of 1 using in. = 0.5 scales ksi of and 101 mm in. = Ma -3 and 2 in.>in. 10 mm From = 0.1(10 the diagram, 3 ) mm/mm. determine From the approximately diagram, determine the modulus approximately of elasticity. the modulus of elasticity. Stress and Strain: Stress and Strain: = e = dl s 5 (ksi) (in./in.) (Ma) e 5 dl L (mm/mm) Load Load (kn) (kip) Contraction (mm) (in.) Modulus of Elasticity: From the stress strain diagram = E 0 approx = B ksi = 26.67(103 ) Ma = Ga 16 s (Ma) (mm/mm) SM_CH08.indd 507 4/11/11 9:54:20 M

2 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently Data taken from a stress strain test for a ceramic are given in the table.the curve is linear between the origin and the first point. lot the diagram, and determine the modulus of elasticity and the modulus of resilience. Modulus of Elasticity: From the stress strain diagram E 5 = = B ksi (103 ) Ma = Ga S (Ma) (ksi) e (mm/mm) (in./in.) Modulus of Resilience: The modulus of resilience is equal to the area under the linear portion of the stress strain diagram (shown shaded). 420 u t = 1 2 (33.2)103 B lb in in in. = 9.96 in # lb u t = 1 2 (232.4)a N mm mm2b a mm b = N mm/mm3 = MJ/m 3 in e (mm/mm) Data taken from a stress strain test for a ceramic are given in the table. The curve is linear between the origin and the first point. lot the diagram, and determine approximately the modulus of toughness. The rupture stress is s r = ksi. Ma Modulus of Toughness: The modulus of toughness is equal to the area under the stress strain diagram (shown shaded). (Ma) S (ksi) e (mm/mm) (in./in.) (33.2)103 B lb in. (u t ) approx = 1 2 ( ) 2 (232.4)a N mm2b( )amm in mm b in B lb in a N 2 (0.0012) mm 2b(0.0012)amm in in. b (7.90)103 B lb in (0.0012) 2 (55.3)a N mm 2b(0.0012)amm in b in. (12.3)103 B lb in (0.0004) 2 (86.1)a N mm 2b(0.0004)amm in b in. = in N # lb mm/mm 3 in 3 = MJ/m 3 s (Ma) e (mm/mm) SM_CH08.indd 508 4/11/11 9:54:20 M

3 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 4. *8 4. tension test was performed on a specimen having an original diameter of 12.5 mm and a gauge length of 50 mm. The data are listed in the table. lot the stress strain diagram, and determine approximately the modulus of elasticity, the ultimate stress, and the fracture stress. Use a scale of 20 mm = 50 Ma and 20 mm = 0.05 mm>mm. Redraw the linear-elastic region, using the same stress scale but a strain scale of 20 mm = mm>mm. Stress and Strain: s = e = dl (Ma) L (mm/mm) Load (kn) Elongation (mm) Modulus of Elasticity: From the stress strain diagram (E) approx = (106 ) = 229 Ga Ultimate and Fracture Stress: From the stress strain diagram (s m ) approx = 528 Ma (s f ) approx = 479 Ma SM_CH08.indd 509 4/11/11 9:54:21 M

4 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently tension test was performed on a steel specimen having an original diameter of 12.5 mm and gauge length of 50 mm. Using the data listed in the table, plot the stress strain diagram, and determine approximately the modulus of toughness. Use a scale of 20 mm = 50 Ma and 20 mm = 0.05 mm>mm. Stress and Strain: s = e = dl (Ma) L (mm/mm) Modulus of Toughness: The modulus of toughness is equal to the total area under the stress strain diagram and can be approximated by counting the number of squares. The total number of squares is 187. Load (kn) Elongation (mm) (u t ) approx = 187(25)10 6 B N m 2 a0.025 m b = 117 MJ>m3 m SM_CH08.indd 510 4/11/11 9:54:21 M

5 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently specimen is originally ft mm long, long, has has a a diameter of of in., mm, and is and subjected is subjected to a force to a of force 500 lb. of When 2.5 kn. the When force the is increased force is increased from 500 lb from to kn lb, the to 9 specimen kn,, the elongates specimen elongates in Determine mm. Determine the modulus the modulus of elasticity of elasticity for the for the material material if it if remains it remains linear linear elastic. elastic. Normal Stress and Strain: pplying s = and e = dl. L s = (103 ) = ksi Ma p 4 (0.52 (12) 2 ) s = (103 ) 5 = Ma ksi p ( (12 2 ) e = e = mm/mm in.>in Modulus of Elasticity: E = s e = 5 = 76.64( ) B Ma ksi = Ga structural member in a nuclear reactor is made of a zirconium alloy. If an axial load of 20 4 kip kn is to be supported by the member, determine its required cross-sectional area. Use a factor of safety of 3 relative to yielding. What is the load on the member if it is 13 m ft long and its elongation is mm? in.? E 14(10 3 zr = 100 Ga, ) ksi, s Y s Y = = Ma. ksi. The material has elastic behavior. llowable Normal Stress: F.S. = s y s allow 3 = s allow s allow = ksi Ma s allow = = 20(103 4 ) = mmin 2 2 = in 2 Stress Strain Relationship: pplying Hooke s law with e = d L = = mm/mm in.>in. 1(10 3 (12) 3 ) s = Ee = = 100( )(0.0005) 3 B ( ) = 50 Ma = ksi Normal Force: pplying equation s =. = s = = 50(150) (0.2087) = 7500 N = kn kip SM_CH08.indd 511 4/11/11 9:54:21 M

6 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 8. *8 8. The strut is supported by a pin at C and an -36 steel guy wire B. If the wire has a diameter of mm, in., determine how much it stretches when the distributed load acts on the strut kn/m lb/ft Here, we are only interested in determining the force in wire B. C ftm B a+ M C = 0; F 60 (9) - B cos 60 (2.7) 1 (200)(9)(3) = lb 2 (3.4)(2.7)(0.9) = 0 F B = 3.06 kn The normal stress the wire is s B = F B B = 3.06( ) p 4 (0.22 p = 19.10(103 ) psi = ksi 4 (5 2 = Ma ) Since s B 6 s y = ksi Ma,, Hooke s Law Law can can be be applied to determine the strain in wire. s B = E B ; = 29.0(10 200(10 3 )e ) B e B B = ( ( ) mm/mm in>in The unstretched length of the wire is stretches 2.7(10 L B = 9(12) 3 ) = inthus,. the the wire wire sin 60 d B = B L B = ( ( )( ) )(124.71) = mm in. 1 (3.4)(2.7) kn m 1.8 m SM_CH08.indd 512 4/11/11 9:54:22 M

7 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The s diagram for a collagen fiber bundle from which a human tendon is composed is shown. If a segment of the chilles tendon at has a a length of of mm in. and an approximate cross-sectional area of mm in 2, determine its elongation if the foot supports a load of lb, N, which causes a tension in the tendon of lb. N. s (Ma) (ksi) s 5 = = 1.50 ksi = Ma From the graph e = mm/mm in.>in Nlb (mm/mm) (in./in.) d = el = 0.035(6.5) 0.035(165) = mm in The The stress-strain stress strain diagram diagram for for a metal metal alloy alloy having having an an original original diameter diameter of of in. mm and and a gauge a gauge length length of 2 of in. 50 is mm given is in given the in figure. the figure. Determine Determine approximately approximately the the modulus modulus of elasticity of elasticity for the for material, the material, the load the on load the on specimen the specimen that causes that yielding, causes yielding, and the ultimate and the load ultimate the specimen load the will specimen support. will support. From the stress strain diagram, Fig. a, E ksi Ma - 0 = ; ; E = 30.0( Ga) ksi s y = ksi Ma s u>t s u/t = = ksi Ga Thus, Y = 60C p Y = s Y = 290[ p 4(12 4 ( )] )D = 32.80(10 = kip ) N = kip kn u>t u>t = 100C p u/t = s u/t = 500[ p 4(124 2 (0.52 )] = 62.20(10 )D = ) N kip = = 19.6 knkip s (ksi) (in./in.) (Ma) y 300 = E B 0 (mm/m) / 0.08/ / / / / / p Elastic Recovery (a) SM_CH08.indd 513 4/11/11 9:54:23 M

8 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The stress strain diagram for a steel alloy having an original diameter of mm in. and a gauge length of 50 2 in. mm is given is given in in the the figure. If If the the specimen is is loaded until it is stressed to ksi, Ma, determine the approximate amount of elastic recovery and the increase in the gauge length after it is unloaded. s (ksi) (in./in.) From the stress strain diagram Fig. a, the modulus of elasticity for the steel alloy is E ksi Ma - 0 = ; E = (103 Ga) ksi when the specimen is unloaded, its normal strain recovered along line B, Fig. a, which has a gradient of E. Thus = 90 E = 90 ksi Elastic Recovery (10 3 = in>in E = 500 Ma = mm/mm 290(10 3 ) Ma ) ksi Thus, the permanent mount of set Elastic is Recovery = (50 mm) = mm Thus, the permanent = set is = in>in Then, the increase in gauge length e = 0.08 is = mm/mm Then, the L increase = L in gauge = 0.047(2) length = is in L = e L = (50 mm) = mm (Ma) E B 0 (mm/mm) / 0.08/ / / / / / p Elastic Recovery (a) SM_CH08.indd 514 4/11/11 9:54:24 M

9 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 12. *8 12. The stress strain diagram for a steel alloy having an original diameter of mm in. and a a gauge length of of 502 mm in. is given in the figure. Determine approximately the modulus of resilience and the modulus of toughness for the material. The Modulus of resilience is equal to the area under the stress strain diagram up to the proportional limit. Thus, s L = ksi Ma L e L = = in>in. mm/mm (u i ) r = 1 2 s L L = 1 2 C60(103 )D(0.002) = 60.0 in # lb [(290)](0.001) = Ma in 3 The modulus of toughness is equal to the area under the entire stress strain diagram. This area can be approximated by counting the number of squares. The total number is Thus. Thus, C(u i ) t D approx = 38 c15(10 3 ) lb in d a in in b = 28.5(103 ) in # lb [(u i ) t ] approx = 33[100 Ma]a0.04 mm b = 132 Ma mm in 3 s (ksi) 105 (Ma) L = E B (in./in.) (mm/m) / / / / / / / (a) SM_CH08.indd 515 4/11/11 9:54:24 M

10 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently bar bar having having a a length length of of 5 in. 125 and mm cross-sectional and crosssectional area of 0.7 area in 2 is of subjected mm to 2 is an subjected axial force to an of 8000 axial lb. force If the of 40 bar kn. stretches If the bar stretches in., determine 0.05 mm, the determine modulus the of elasticity modulus of of the elasticity material. of the The material. material The has linear-elastic material has behavior. linear-elastic behavior knlb in. mm knlb Normal Stress and Strain: s 5 = 8.00 = ksi = 40(103 ) Ma e 5 = dl = in.>in. L = mm/mm 1255 Modulus of Elasticity: = E 5 s = 28.6(103 ) ksi e = (103 ) Ma = Ga The rigid pipe is supported by a pin at and an -36 steel guy wire BD. If the wire has a diameter of mm, in., determine how much it it stretches when a load of = 3600 kn acts lb acts on on the the pipe. pipe. B Here, we are only interested in determining the force in wire BD. Referring to the FBD in Fig. a ftm a+ M = 0; F BD 4 5 B(3) (0.9)- 600(6) 3(1.8) = 0 F BD BD = = kn lb The normal stress developed in the wire is s BD = F BD BD = 7.5( ) pp 4 (0.252 ) = 30.56(103 ) psi = ksi 4 ( Ma ) D ftm ftm C Since s BD 6 s y = ksi Ma,, Hooke s Law Law can can be be applied to to determine the the strain in in the wire. s BD = E BD ; = 200( (10 3 )e 3 ) B BD BD e = 1.054(10-3 BD = (10 3 ) ) in.>in. mm/mm The unstretched length of the wire is wire stretches 2 2 L BD = = = 5ft 1.5 = m. 60 Thus, in. Thus, the the d BD = BD L BD = ( ( )(60) )(1.5)(10 3 ) = inmm 3 kn 0.9 m 0.9 m SM_CH08.indd 516 4/11/11 9:54:25 M

11 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The rigid pipe is supported by a pin at and an -36 guy wire BD. If the wire has a a diameter of of mm, in., determine the load if the end C is is displaced mm in. downward. B ftm D ftm ftm C Here, we are only interested in determining the force in wire BD. Referring to the FBD in Fig. a a+ M = 0; F BD 4 5 B(3) (0.9)- (6) (1.8) = = 00 F BD = 2.50 The unstretched length for wire BD is L BD = = = 51.5 ft m. = 60 From in. From the the geometry shown in Fig. b, the stretched length of wire BD is 2 2 L BD = (60)(0.075) ( ) cos = = mm Thus, the normal strain is BD = L BD - L BD L BD = Then, the normal stress can be obtain by applying Hooke s Law. s BD = E BD = 200(10 29(10 3 )C1.0003(10 3 )[1.0000( )D )] = Ma ksi Since s BD 6 s y = ksi Ma,, the the result result is valid. is valid = ( ( ) 3 ) mm/mm in.>in s BD = F BD ; 29.01( p 3 ) = BD 4 (6 2 ) 2.50 p 4 (0.252 ) = N lb = = knlb L BD = 1.5 m 0.9 m 0.9 m mm SM_CH08.indd 517 4/11/11 9:54:26 M

12 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 16. *8 16. Determine the elongation of the square hollow bar when it is subjected to the axial force = 100 kn. If this axial force is increased to = 360 kn and released, find the permanent elongation of the bar. The bar is made of a metal alloy having a stress strain diagram which can be approximated as shown. s (Ma) mm 50 mm mm (mm/mm) 50 mm 5 mm Normal Stress and Strain: The cross-sectional area of the hollow bar is = = 0.9(10-3 )m 2. When = 100 kn, s 1 = = 100(103 ) 0.9(10-3 = Ma ) From the stress strain diagram shown in Fig. a, the slope of the straight line O which represents the modulus of elasticity of the metal alloy is E = 250(106 ) = 200 Ga Since s Ma, Hooke s Law can be applied. Thus s 1 = Ee 1 ; (10 6 ) = 200(10 9 )e 1 e 1 = (10-3 ) mm>mm Thus, the elongation of the bar is d 1 = e 1 L = (10-3 )(600) = mm When = 360 kn, s 2 = = 360(103 ) 0.9(10-3 = 400 Ma ) From the geometry of the stress strain diagram, Fig. a, e = e 2 = mm>mm When = 360 kn is removed, the strain recovers linearly along line BC, Fig. a, parallel to O. Thus, the elastic recovery of strain is given by s 2 = Ee r ; 400(10 6 ) = 200(10 9 )e r e r = mm>mm The permanent set is e = e 2 - e r = = mm>mm Thus, the permanent elongation of the bar is d = e L = (600) = 17.1 mm SM_CH08.indd 518 4/11/11 9:54:26 M

13 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently Continued SM_CH08.indd 519 4/11/11 9:54:26 M

14 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently tension test was performed on an aluminum 2014-T6 alloy specimen. The resulting stress strain diagram is shown in the figure. Estimate (a) the proportional limit, (b) the modulus of elasticity, and (c) the yield strength based on a 0.2% strain offset method. s (ksi) (Ma) (mm/mm) (in./in.) roportional Limit and Yield Strength: From the stress strain diagram, Fig. a, s pl = ksi Ma s Y = ksi Ma Modulus of Elasticity: From the stress strain diagram, the corresponding strain for s L = ksi Ma is is e pl e pl = = in.>in. mm/mm. Thus, Thus, E 5 = = 11.0(103 ) ksi (103 ) Ma = 77.0 Ga Modulus of Resilience: The modulus of resilience is equal to the area under the s (Ma) e (mm/mm) SM_CH08.indd 520 4/11/11 9:54:27 M

15 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently tension test was performed on an aluminum 2014-T6 alloy specimen. The resulting stress strain diagram is shown in the figure. Estimate (a) the modulus of resilience; and (b) modulus of toughness. s (Ma) (ksi) (mm/mm) (in./in.) stress strain diagram up to the proportional limit. From the stress strain diagram, s pl = ksi Ma e pl = mm/mm in.>in. Thus, U i B r = 1 2 s ple pl = 1 2 (44)(103 )(0.004) = 88 in # lb (308)(0.004) = MJ/m 3 in 3 Modulus of Toughness: The modulus of toughness is equal to the area under the entire stress strain diagram. This area can be approximated by counting the number of squares. The total number of squares is 65. Thus, CU i B t D approx = 65B10(10 3 ) lb in R 2 c0.01in. in. d = 6.50(103 ) in # lb 65[70 Ma]c 0.01 mm d = 45.5 MJ/m3 mm in 3 The stress strain diagram for a bone is shown, and can be described by the equation The stress strain diagram for a bone is shown, and can be described by the equation = s s 3, where s is in ka. Determine the yield strength assuming a 0.3% offset. s 0.45(10 6 )s (10 12 )s 3 e = 0.45(10-6 )s (10-12 )s 3, d =0.45(10-6 ) (10-12 ) s 2 Bds E = ds d 2 s = 0 1 = = 2.22 Ma 0.45(10-6 ) SM_CH08.indd 521 4/11/11 9:54:27 M

16 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 20. *8 20. The stress strain diagram for a bone is shown and can be described by the equation = s s 3, where s is in ka. Determine the modulus of toughness and the amount of elongation of a 200-mmlong region just before it fractures if failure occurs at =0.12 mm>mm. s 0.45(10 6 )s (10 12 )s 3 When e = (10 3 ) = 0.45 s (10-6 )s 3 Solving for the real root: s = ka u t = d = ( e)ds L L u t = ( (10-6 )s (10-12 )s 3 )ds L 0 0 = 0.12 s (10-6 )s (10-12 )s = 613 kj>m 3 d = el = 0.12(200) = 24 mm SM_CH08.indd 522 4/11/11 9:54:27 M

17 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The acrylic plastic rod is 200 mm long and 15 mm in diameter. If an axial load of 300 N is applied to it, determine the change in its length and the change in its diameter. E p = 2.70 Ga, n p = N 200 mm 300 N s = = 300 p 4 (0.015)2 = Ma e long = s E = 1.697(106 ) 2.70(10 9 ) = d = e long L = (200) = mm e lat = -Ve long = -0.4( ) = d = e lat d = (15) = mm 523 SM_CH08.indd 523 4/11/11 9:54:28 M

18 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The short cylindrical block of 2014-T6 aluminum, having an original diameter of of mm in. and a a length of of mm, in., is placed in the smooth jaws of a vise and squeezed until the axial load applied is kn. lb. Determine (a) the decrease in its length and (b) its new diameter knlb knlb a) = 800 s 5 = psi = 4(10 3 ) p 4 (12 (0.5) Ma ) 4 e = (10 6 ) = long 5 s E = (10 6 ) d 5 = e = (1.5) = (10-3 long L (37.5) mm ) in. b) V = -e lat y = 0.35 e long e lat = ( ) ( ) = = d = e lat d = (12) (0.5) = = mm d =d + d = mm in The elastic portion of the stress strain diagram for a steel alloy is shown in the figure. The specimen from which it was obtained had an original diameter of 13 mm and a gauge length of 50 mm. When the applied load on the specimen is 50 kn, the diameter is mm. Determine oisson s ratio for the material. s(ma) 400 Normal Stress: s = = 50(103 ) p = Mpa 4 ( ) (mm/mm) Normal Strain: From the stress strain diagram, the modulus of elasticity E = 400(106 ) = 200 Ga. pplying Hooke s law e long = s E = (106 ) 200(10 4 ) = B mm>mm e lat = d - d = = B mm>mm d 0 13 oisson s Ratio: The lateral and longitudinal strain can be related using oisson s ratio. V = - e lat e long = (10-3 ) (10-3 ) = SM_CH08.indd 524 4/11/11 9:54:29 M

19 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 28. *8 24. The elastic portion of the stress strain diagram for a steel alloy is shown in the figure. The specimen from which it was obtained had an original diameter of 13 mm and a gauge length of 50 mm. If a load of = 20 kn is applied to the specimen, determine its diameter and gauge length. Take n = 0.4. s(ma) 400 Normal Stress: s = = 20(103 ) p 4 ( ) = Mpa (mm/mm) Normal Strain: From the Stress Strain diagram, the modulus of elasticity E = 400(106 ) = 200 Ga. pplying Hooke s Law e long = s E = (106 ) 200(10 9 ) = B mm>mm Thus, dl = e long L 0 = B(50) = mm L = L 0 + dl = = mm oisson s Ratio: The lateral and longitudinal can be related using poisson s ratio. e lat = -ve long = -0.4(0.7534)10-3 B = B mm>mm dd = e lat d = B(13) = mm d = d 0 + dd = 13 + ( ) = mm The aluminum block has a rectangular cross section and is subjected to an axial compressive force of 840 kip. kn. If the 37.5-mm 1.5-in. side side changed its its length to mm, in., determine oisson s ratio and the new length of of the the 502-in. mm side. E 10(10 3 al = 70 Ga. ) ksi mmin. 8 kip 2 in. 40 kn 50 mm 40 8 kip kn 753 mm in. = 8 s 5 = ksi = 40(10 3 ) Ma (50)(37.5) (2)(1.5) e = long 5 s E = (10 10(10 3 ) 3 ) 5 = e lat 5 = 5 = v 5 = = h h9 5 = (50) (2) = mm in SM_CH08.indd 525 4/11/11 9:54:34 M

20 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The block is made of titanium Ti-61-4V and is subjected to a compression of mm in. along the y axis, and its shape is given a tilt of u = Determine x, y, and g xy. y Normal Strain: e y = dl y 1.5 = = mm/mm in.>in. L y oisson s Ratio: The lateral and longitudinal strain can be related using oisson s ratio mm in. u in. mm x e x = -ve y = -0.36( ) = in. mm/mm >in. Shear Strain: b = = 90.3 = rad g xy = p 2 - b = p = rad The shear stress strain diagram for a steel alloy is shown in the figure. If a bolt having a diameter of mm in. is made of this material and used in the double lap joint, determine the modulus of elasticity E and the force required to cause the material to yield. Take n = 0.3. The shear force developed on the shear planes of the bolt can be determined by considering the equilibrium of the FBD shown in Fig. a : + F x = 0; V + V - = 0 V = = 2 2 From the shear stress strain diagram, the yield stress is t y = ksi Ma.. Thus, Thus, t y = V y ; 60 = /2 > p p 4 ( ) B t(ma) t(ksi) /2 /2 g(rad) = kip N = kipkn From the shear stress strain diagram, the shear modulus is Thus, the modulus of elasticity is ksi G 5 = = 11.01(103 ksi (103 ) Ma Ga G = E 2(1 + y) ; 11.01( ) = E 2( ) E = E 28.6( ) Ga ksi SM_CH08.indd 526 4/11/11 9:54:38 M

21 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *8 28. *3 32. shear spring is made by bonding the rubber annulus to a rigid fixed ring and a plug. When an axial load is placed on the plug, show that the slope at point y in the rubber is dy>dr =-tan g = - tan1>12phgr22. For small angles we can write dy>dr = ->12phGr2. Integrate this expression and evaluate the constant of integration using the condition that y = 0 at r = r o. From the result compute the deflection y = d of the plug. r o d r i r y h y Shear Stress Strain Relationship: pplying Hooke s law with t =. 2p r h g = t G = 2p h G r dy dr = -tan g = -tan a 2p h G r b (Q.E.D) If g is small, then tan g = g. Therefore, t r = r o, y = 0 Then, y = 2p h G ln r o r t r = r i, y = d dy dr = - 2p h G r dr y = - 2p h G L r y = - 0 = - C = 2p h G ln r + C 2p h G ln r o + C 2p h G ln r o d = 2p h G ln r o r i SM_CH08.indd 527 4/11/11 9:54:39 M

22 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The support consists of three rigid plates, which are connected together using two symmetrically placed rubber pads. If a vertical force of 5 N is applied to plate, determine the approximate vertical displacement of this plate due to shear strains in the rubber. Each pad has cross-sectional dimensions of 30 mm and 20 mm. G r = 0.20 Ma. C 40 mm B 40 mm t avg = V = 2.5 = a (0.03)(0.02) 5 N g = t G = = rad 0.2(10 6 ) d = 40( ) = mm shear spring is made from two blocks of rubber, each having a height h, width b, and thickness a. The blocks are bonded to three plates as shown. If the plates are rigid and the shear modulus of the rubber is G, determine the displacement of plate if a vertical load is applied to this plate. ssume that the displacement is small so that d = a tan g L ag. d h verage Shear Stress: The rubber block is subjected to a shear force of V =. 2 Shear Strain: pplying Hooke s law for shear Thus, t = V = g = t G = 2 b h = 2 b h 2 b h G = 2 b h G a a d = a g = = a 2 b h G SM_CH08.indd 528 4/11/11 9:54:40 M

23 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The elastic portion of the tension stress strain diagram for an aluminum alloy is shown in the figure. The specimen used for the test has a gauge length of 50 2 in. mm and and a a diameter of of in. mm. When When the applied the applied load load is 9 kip, is 45 the kn, new the diameter new diameter of the of specimen the specimen is is in. Compute mm. Compute the shear the modulus shear modulus for Gthe al for aluminum. the aluminum. G al From the stress strain diagram, = = 70 E al 5 s = ksi e (103 ) Ma When specimen is loaded with a 945-kN - kip load, = = 9 s 5 = ksi 5 45(103 ) p Ma 4 (12.5) (0.5)2 = = e long 5 s = in.>in. E ( mm/mm ) = d -d e lat 5 d9 d = 5 = mm/mm in.>in. d e lat V 5 = - e lat e 5 = - e long = long s(ksi) s (Ma) (mm/mm) (in./in.) E at = v) = 11.4(10 at G 2( ) = 4.31(103 al 5 ) ksi 2(1 + v) (10 3 ) 2( ) (103 ) Ma Ga *3 36. *8 32. The elastic portion of the tension stress strain diagram for an aluminum alloy is shown in the figure. The specimen used for the test has a a gauge length of of 502 mm in. and a diameter of in. mm. If If the the applied load is is kip, kn, determine the new diameter of the specimen. The shear modulus is G al = 28 Ga. 2 ksi. = = s 5 = ksi 5 50(103 ) p Ma 4 (12.5) (0.5)2 4 From the stress-strain stress strain diagram E 5 = = ksi (103 ) Ma e = long 5 s = in.>in. E = ( mm/mm ) E G 5 = v) ; 3.8(103 ) = (1 + v) ; 28(103 ) (103 ) ; v 2(1 + v) ; (1 + v) v = e lat 5 = ve - ve long long 5 = ( ) ( ) 5 = in.>in. d d 5 = ee lat lat d d 5 = (12.5) (0.5) 5 = mm in. s(ksi) s (Ma) (mm/mm) (in./in.) d9 d 5 =d d + + d d 5 = = mmin SM_CH08.indd 529 4/11/11 9:54:41 M

24 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The s diagram for elastic fibers that make up human skin and muscle is shown. Determine the modulus of elasticity of the fibers and estimate their modulus of toughness and modulus of resilience. s(ma) s(psi) (in./in.) (mm/mm) E = 11 al 5 77 = psi Ma 22 u = (2)(11) 1 t 5 1 ( )(2.25-2) = psi 2 (2)(77) + 1 ( )(2.25 2) MJ/m3 2 2 u = t 5 1 (2)(77) (2)(11) 5 = MJ/m3 psi short cylindrical block of 6061-T6 aluminum, having an original diameter of 20 mm and a length of 75 mm, is placed in a compression machine and squeezed until the axial load applied is 5 kn. Determine (a) the decrease in its length and (b) its new diameter. a) s = = -5(103 ) p 4 (0.02)2 = Ma s = E e long ; (10 6 ) = 68.9(10 9 ) e long e long = mm>mm d = e long L = (75) = mm b) e lat e lat v = - ; 0.35 = - e long e lat = mm>mm d = e lat d = (20) = mm d =d + d = = mm SM_CH08.indd 530 4/11/11 9:54:42 M

25 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The rigid beam rests in the horizontal position on two 2014-T6 aluminum cylinders having the unloaded lengths shown. If each cylinder has a diameter of 30 mm, determine the placement x of the applied 80-kN load so that the beam remains horizontal. What is the new diameter of cylinder after the load is applied? n al = mm x 80 kn B 210 mm a + M = 0; F B (3) - 80(x) = 0; F B = 80x (1) 3 3 m 80(3 - x) a + M B = 0; -F (3) + 80(3 - x) = 0; F = (2) 3 Since the beam is held horizontally, d = d B s = ; e = s E = E d = el = a E b L = L E 80(3 - x) 3 (220) d = d B ; = E 80(3 - x)(220) = 80x(210) 80x 3 (210) E x = 1.53 m From Eq. (2), F = kn s = F = 39.07(103 ) p = Ma 4 (0.032 ) e long = s E = (106 ) 73.1(10 9 ) = e lat = -ve long = -0.35( ) = d œ = d + d e lat = ( ) = mm *3 40. *8 36. The head H is connected to the cylinder of a compressor using six steel bolts. If the clamping force in each bolt is is 4800 kn, lb, determine the the normal normal strain strain the in bolts. the 3 bolts. Each Each bolt has bolt a has diameter a diameter of 5 of mm. If s Y = 40 ksi If in. s Y = 280 Ma and H E st = 200 Ga, 2 ksi, what what is the is strain the strain each in each bolt when bolt when the nut the is nut unscrewed is unscrewed so that so the that clamping the clamping force is force released? is released? LC Normal Stress: s 5 = = B = ksi 6 2 = 40 ksi 5 4(103 ) p 4 (5) Ma < s g Ma Normal Strain: Since s 6 s g, Hooke s law is still valid. e 5 = s = (10 3 = in.>in. E mm/mm 200(10) ) If the nut is unscrewed, the load is zero. Therefore, the strain e = SM_CH08.indd 531 4/11/11 9:54:42 M

26 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The stone has a mass of 800 kg and center of gravity at G. It rests on a pad at and a roller at B.The pad is fixed to the ground and has a compressed height of 30 mm, a width of 140 mm, and a length of 150 mm. If the coefficient of static friction between the pad and the stone is m s = 0.8, determine the approximate horizontal displacement of the stone, caused by the shear strains in the pad, before the stone begins to slip. ssume the normal force at acts 1.5 m from G as shown. The pad is made from a material having E = 4 Ma and n = m B G 1.25 m 1.5 m 0.3 m Equations of Equilibrium: a + M B = 0; F (2.75) (1.25) - (0.3) = 0 [1] : + F x = 0; - F = 0 [2] Note: The normal force at does not act exactly at. It has to shift due to friction. Friction Equation: F = m s F = 0.8 F [3] Solving Eqs. [1], [2] and [3] yields: verage Shear Stress: The pad is subjected to a shear force of V = F = N. Modulus of Rigidity: F = N F = = N G = t = V = = ka (0.14)(0.15) E 2(1 + v) = 4 = Ma 2( ) Shear Strain: pplying Hooke s law for shear g = t G = (103 ) 1.481(10 6 ) = rad Thus, d h = hg = 30(0.1005) = 3.02 mm SM_CH08.indd 532 4/11/11 9:54:43 M

27 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently The bar D is rigid and is originally held in the horizontal position when the weight W is supported from C. E If the weight causes B to be displaced downward mm, in., determine the strain in wires DE and BC. lso, if the wires 0.93 mft are made of -36 steel and have a cross-sectional area of mm in 22,, determine the weight W ft m ft m D B = 1.5 d ft m d = in mm C e DE = d = in.>in. L = = mm/mm 0.9(1000) 3(12) W s = 29(10 3 DE = Ee DE = 200(10 3 )( ) )( ) = = ksi Ma F DE = s DE DE DE DE = = (1.25) (0.002) = = N kip a+ M = 0; (289.35)(1.5) -(0.0672) (5) + 0.9(W) 3(W) = m 0.9 m W = kip N = 112 lb s BC = BC = W = = = Ma ksi BC 1.25 BC e BC BC = BC = s BC E = (10 29 (10 3 = 3 = ) mm/mm in.>in. ) F DE = N 0.6 m 0.9 m The 8-mm-diameter bolt is made of an aluminum alloy. It fits through a magnesium sleeve that has an inner diameter of 12 mm and an outer diameter of 20 mm. If the original lengths of the bolt and sleeve are 80 mm and 50 mm, respectively, determine the strains in the sleeve and the bolt if the nut on the bolt is tightened so that the tension in the bolt is 8 kn. ssume the material at is rigid. E al = 70 Ga, E mg = 45 Ga. 50 mm 30 mm Normal Stress: s b = b = 8(10 3 ) p = Ma 4 ( ) s s = 8(10 3 ) = p s 4 ( = Ma ) Normal Strain: pplying Hooke s Law e b = s b E al = (106 ) 70(10 9 ) e s = = mm>mm s s = 39.79(106 ) E mg 45(10 9 = mm>mm ) SM_CH08.indd 533 4/11/11 9:54:44 M

28 2011 earson Education, Inc., Upper Saddle River, NJ. ll rights reserved. This material is protected under all copyright laws as they currently *3 44. *8 40. The -36 steel wire B has a cross-sectional area of 10 mm 2 and is unstretched when u = Determine the applied load needed to cause u = mm u 400 mm B L B sin 90.2 = 400 sin 44.9 L B = mm L B = e = L B - L B = = L B s = Ee = 200(10 9 ) ( ) = Ma a+ M = sin 45 = (400 cos 0.2 ) - F B sin 44.9 (400) = 0 (1) However, F B = s = (10 6 )(10)(10-6 ) = kn From Eq. (1), = 2.46 kn SM_CH08.indd 534 4/11/11 9:54:44 M

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3 MECE 3321 MECHANICS OF SOLIDS CHAPTER 3 Samantha Ramirez TENSION AND COMPRESSION TESTS Tension and compression tests are used primarily to determine the relationship between σ avg and ε avg in any material.

More information

The University of Melbourne Engineering Mechanics

The University of Melbourne Engineering Mechanics The University of Melbourne 436-291 Engineering Mechanics Tutorial Four Poisson s Ratio and Axial Loading Part A (Introductory) 1. (Problem 9-22 from Hibbeler - Statics and Mechanics of Materials) A short

More information

[5] Stress and Strain

[5] Stress and Strain [5] Stress and Strain Page 1 of 34 [5] Stress and Strain [5.1] Internal Stress of Solids [5.2] Design of Simple Connections (will not be covered in class) [5.3] Deformation and Strain [5.4] Hooke s Law

More information

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2 Samantha Ramirez, MSE Stress The intensity of the internal force acting on a specific plane (area) passing through a point. Δ ΔA Δ z Δ 1 2 ΔA Δ x Δ y ΔA is an infinitesimal size area with a uniform force

More information

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3.

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3. ES230 STRENGTH OF MTERILS Exam 3 Study Guide Exam 3: Wednesday, March 8 th in-class Updated 3/3/17 Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on

More information

Stress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y.

Stress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y. 014 Pearson Education, Inc., Upper Saddle River, NJ. All rights reserved. This material is protected under all copyright laws as they currently 9 7. Determine the normal stress and shear stress acting

More information

4.MECHANICAL PROPERTIES OF MATERIALS

4.MECHANICAL PROPERTIES OF MATERIALS 4.MECHANICAL PROPERTIES OF MATERIALS The diagram representing the relation between stress and strain in a given material is an important characteristic of the material. To obtain the stress-strain diagram

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading MA 3702 Mechanics & Materials Science Zhe Cheng (2018) 2 Stress & Strain - Axial Loading Statics

More information

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts. NORMAL STRESS The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts. σ = force/area = P/A where σ = the normal stress P = the centric

More information

INTRODUCTION TO STRAIN

INTRODUCTION TO STRAIN SIMPLE STRAIN INTRODUCTION TO STRAIN In general terms, Strain is a geometric quantity that measures the deformation of a body. There are two types of strain: normal strain: characterizes dimensional changes,

More information

Mechanical properties 1 Elastic behaviour of materials

Mechanical properties 1 Elastic behaviour of materials MME131: Lecture 13 Mechanical properties 1 Elastic behaviour of materials A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka Today s Topics Deformation of material under the action of a mechanical

More information

Mechanical Properties of Materials

Mechanical Properties of Materials Mechanical Properties of Materials Strains Material Model Stresses Learning objectives Understand the qualitative and quantitative description of mechanical properties of materials. Learn the logic of

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third CHTR Stress MCHNICS OF MTRIS Ferdinand. Beer. Russell Johnston, Jr. John T. DeWolf ecture Notes: J. Walt Oler Texas Tech University and Strain xial oading Contents Stress & Strain: xial oading Normal

More information

Determine the resultant internal loadings acting on the cross section at C of the beam shown in Fig. 1 4a.

Determine the resultant internal loadings acting on the cross section at C of the beam shown in Fig. 1 4a. E X M P L E 1.1 Determine the resultant internal loadings acting on the cross section at of the beam shown in Fig. 1 a. 70 N/m m 6 m Fig. 1 Support Reactions. This problem can be solved in the most direct

More information

Stress-Strain Behavior

Stress-Strain Behavior Stress-Strain Behavior 6.3 A specimen of aluminum having a rectangular cross section 10 mm 1.7 mm (0.4 in. 0.5 in.) is pulled in tension with 35,500 N (8000 lb f ) force, producing only elastic deformation.

More information

ME 243. Mechanics of Solids

ME 243. Mechanics of Solids ME 243 Mechanics of Solids Lecture 2: Stress and Strain Ahmad Shahedi Shakil Lecturer, Dept. of Mechanical Engg, BUET E-mail: sshakil@me.buet.ac.bd, shakil6791@gmail.com Website: teacher.buet.ac.bd/sshakil

More information

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS 3 rd Edition Michael S. Mamlouk Arizona State University John P. Zaniewski West Virginia University Solution Manual FOREWORD This solution manual includes

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third CHTR Stress MCHNICS OF MTRIS Ferdinand. Beer. Russell Johnston, Jr. John T. DeWolf ecture Notes: J. Walt Oler Texas Tech University and Strain xial oading Contents Stress & Strain: xial oading Normal

More information

Solid Mechanics Chapter 1: Tension, Compression and Shear

Solid Mechanics Chapter 1: Tension, Compression and Shear Solid Mechanics Chapter 1: Tension, Compression and Shear Dr. Imran Latif Department of Civil and Environmental Engineering College of Engineering University of Nizwa (UoN) 1 Why do we study Mechanics

More information

NAME: Given Formulae: Law of Cosines: Law of Sines:

NAME: Given Formulae: Law of Cosines: Law of Sines: NME: Given Formulae: Law of Cosines: EXM 3 PST PROBLEMS (LESSONS 21 TO 28) 100 points Thursday, November 16, 2017, 7pm to 9:30, Room 200 You are allowed to use a calculator and drawing equipment, only.

More information

STANDARD SAMPLE. Reduced section " Diameter. Diameter. 2" Gauge length. Radius

STANDARD SAMPLE. Reduced section  Diameter. Diameter. 2 Gauge length. Radius MATERIAL PROPERTIES TENSILE MEASUREMENT F l l 0 A 0 F STANDARD SAMPLE Reduced section 2 " 1 4 0.505" Diameter 3 4 " Diameter 2" Gauge length 3 8 " Radius TYPICAL APPARATUS Load cell Extensometer Specimen

More information

Mechanics of Materials

Mechanics of Materials Mechanics of Materials Notation: a = acceleration = area (net = with holes, bearing = in contact, etc...) SD = allowable stress design d = diameter of a hole = calculus symbol for differentiation e = change

More information

Solid Mechanics Homework Answers

Solid Mechanics Homework Answers Name: Date: Solid Mechanics Homework nswers Please show all of your work, including which equations you are using, and circle your final answer. Be sure to include the units in your answers. 1. The yield

More information

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)?

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)? IDE 110 S08 Test 1 Name: 1. Determine the internal axial forces in segments (1), (2) and (3). (a) N 1 = kn (b) N 2 = kn (c) N 3 = kn 2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS CHATR Stress MCHANICS OF MATRIALS and Strain Axial Loading Stress & Strain: Axial Loading Suitability of a structure or machine may depend on the deformations in the structure as well as the stresses induced

More information

Tensile stress strain curves for different materials. Shows in figure below

Tensile stress strain curves for different materials. Shows in figure below Tensile stress strain curves for different materials. Shows in figure below Furthermore, the modulus of elasticity of several materials effected by increasing temperature, as is shown in Figure Asst. Lecturer

More information

ME 2570 MECHANICS OF MATERIALS

ME 2570 MECHANICS OF MATERIALS ME 2570 MECHANICS OF MATERIALS Chapter III. Mechanical Properties of Materials 1 Tension and Compression Test The strength of a material depends on its ability to sustain a load without undue deformation

More information

Chapter 4-b Axially Loaded Members

Chapter 4-b Axially Loaded Members CIVL 222 STRENGTH OF MATERIALS Chapter 4-b Axially Loaded Members AXIAL LOADED MEMBERS Today s Objectives: Students will be able to: a) Determine the elastic deformation of axially loaded member b) Apply

More information

Russell C. Hibbeler. Chapter 1: Stress

Russell C. Hibbeler. Chapter 1: Stress Russell C. Hibbeler Chapter 1: Stress Introduction Mechanics of materials is a study of the relationship between the external loads on a body and the intensity of the internal loads within the body. This

More information

Constitutive Equations (Linear Elasticity)

Constitutive Equations (Linear Elasticity) Constitutive quations (Linear lasticity) quations that characterize the physical properties of the material of a system are called constitutive equations. It is possible to find the applied stresses knowing

More information

Mechanical Design in Optical Engineering. For a prismatic bar of length L in tension by axial forces P we have determined:

Mechanical Design in Optical Engineering. For a prismatic bar of length L in tension by axial forces P we have determined: Deformation of Axial Members For a prismatic bar of length L in tension by axial forces P we have determined: σ = P A δ ε = L It is important to recall that the load P must act on the centroid of the cross

More information

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering Mechanics Of Solids Suraj kr. Ray (surajjj2445@gmail.com) Department of Civil Engineering 1 Mechanics of Solids is a branch of applied mechanics that deals with the behaviour of solid bodies subjected

More information

MECHANICS OF MATERIALS

MECHANICS OF MATERIALS Third E CHAPTER 2 Stress MECHANICS OF MATERIALS Ferdinand P. Beer E. Russell Johnston, Jr. John T. DeWolf Lecture Notes: J. Walt Oler Texas Tech University and Strain Axial Loading Contents Stress & Strain:

More information

CONTENTS. To the Instructor. 1 Stress 1. 2 Strain Mechanical Properties of Materials Axial Load Torsion 214.

CONTENTS. To the Instructor. 1 Stress 1. 2 Strain Mechanical Properties of Materials Axial Load Torsion 214. FM_TO 46060 6/22/10 11:26 M Page iii ONTENTS To the Instructor iv 1 Stress 1 2 Strain 73 3 Mechanical Proerties of Materials 92 4 xial Load 122 5 Torsion 214 6 ending 329 7 Transverse Shear 472 8 ombined

More information

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola MECHANICS OF MATERIALS Prepared by Engr. John Paul Timola Mechanics of materials branch of mechanics that studies the internal effects of stress and strain in a solid body. stress is associated with the

More information

Introduction to Engineering Materials ENGR2000. Dr. Coates

Introduction to Engineering Materials ENGR2000. Dr. Coates Introduction to Engineering Materials ENGR2 Chapter 6: Mechanical Properties of Metals Dr. Coates 6.2 Concepts of Stress and Strain tension compression shear torsion Tension Tests The specimen is deformed

More information

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS CHAPTER THE EFFECTS OF FORCES ON MATERIALS EXERCISE 1, Page 50 1. A rectangular bar having a cross-sectional area of 80 mm has a tensile force of 0 kn applied to it. Determine the stress in the bar. Stress

More information

3 A y 0.090

3 A y 0.090 ROBLM.1 5.0 in. 5 8 in. diameter A standard tension test is used to determine the properties of an experimental plastic. The test specimen is a 5 -in.-diameter rod and it is subjected to an 800-lb tensile

More information

Mechanics of Materials Primer

Mechanics of Materials Primer Mechanics of Materials rimer Notation: A = area (net = with holes, bearing = in contact, etc...) b = total width of material at a horizontal section d = diameter of a hole D = symbol for diameter E = modulus

More information

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy Stress Analysis Lecture 3 ME 276 Spring 2017-2018 Dr./ Ahmed Mohamed Nagib Elmekawy Axial Stress 2 Beam under the action of two tensile forces 3 Beam under the action of two tensile forces 4 Shear Stress

More information

MECE 3321: Mechanics of Solids Chapter 6

MECE 3321: Mechanics of Solids Chapter 6 MECE 3321: Mechanics of Solids Chapter 6 Samantha Ramirez Beams Beams are long straight members that carry loads perpendicular to their longitudinal axis Beams are classified by the way they are supported

More information

Free Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2

Free Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2 Problem 10.9 The angle β of the system in Problem 10.8 is 60. The bars are made of a material that will safely support a tensile normal stress of 8 ksi. Based on this criterion, if you want to design the

More information

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and 6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa (15.5 10 6 psi) and an original diameter of 3.8 mm (0.15 in.) will experience only elastic deformation when a tensile

More information

Stress Strain Elasticity Modulus Young s Modulus Shear Modulus Bulk Modulus. Case study

Stress Strain Elasticity Modulus Young s Modulus Shear Modulus Bulk Modulus. Case study Stress Strain Elasticity Modulus Young s Modulus Shear Modulus Bulk Modulus Case study 2 In field of Physics, it explains how an object deforms under an applied force Real rigid bodies are elastic we can

More information

COLUMNS: BUCKLING (DIFFERENT ENDS)

COLUMNS: BUCKLING (DIFFERENT ENDS) COLUMNS: BUCKLING (DIFFERENT ENDS) Buckling of Long Straight Columns Example 4 Slide No. 1 A simple pin-connected truss is loaded and supported as shown in Fig. 1. All members of the truss are WT10 43

More information

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion Introduction Stress and strain in components subjected to torque T Circular Cross-section shape Material Shaft design Non-circular

More information

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY Spring 2006 Final Examination STUDENT S NAME (please print) STUDENT S SIGNATURE STUDENT NUMBER IDE 110 CLASS SECTION INSTRUCTOR S NAME Do not turn this page until instructed to start. Write your name on

More information

Problem " Â F y = 0. ) R A + 2R B + R C = 200 kn ) 2R A + 2R B = 200 kn [using symmetry R A = R C ] ) R A + R B = 100 kn

Problem  Â F y = 0. ) R A + 2R B + R C = 200 kn ) 2R A + 2R B = 200 kn [using symmetry R A = R C ] ) R A + R B = 100 kn Problem 0. Three cables are attached as shown. Determine the reactions in the supports. Assume R B as redundant. Also, L AD L CD cos 60 m m. uation of uilibrium: + " Â F y 0 ) R A cos 60 + R B + R C cos

More information

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work. It is most beneficial to you to write this mock final exam UNDER EXAM CONDITIONS. This means: Complete the exam in 3 hours. Work on your own. Keep your textbook closed. Attempt every question. After the

More information

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor.

1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor. Elasticity Homework Problems 2014 Section 1. The Strain Tensor. 1. A pure shear deformation is shown. The volume is unchanged. What is the strain tensor. 2. Given a steel bar compressed with a deformation

More information

Solution: T, A1, A2, A3, L1, L2, L3, E1, E2, E3, P are known Five equations in five unknowns, F1, F2, F3, ua and va

Solution: T, A1, A2, A3, L1, L2, L3, E1, E2, E3, P are known Five equations in five unknowns, F1, F2, F3, ua and va ME 323 Examination # 1 February 18, 2016 Name (Print) (Last) (First) Instructor PROBLEM #1 (20 points) A structure is constructed from members 1, 2 and 3, with these members made up of the same material

More information

Strength of Materials (15CV 32)

Strength of Materials (15CV 32) Strength of Materials (15CV 32) Module 1 : Simple Stresses and Strains Dr. H. Ananthan, Professor, VVIET,MYSURU 8/21/2017 Introduction, Definition and concept and of stress and strain. Hooke s law, Stress-Strain

More information

STRESS. Bar. ! Stress. ! Average Normal Stress in an Axially Loaded. ! Average Shear Stress. ! Allowable Stress. ! Design of Simple Connections

STRESS. Bar. ! Stress. ! Average Normal Stress in an Axially Loaded. ! Average Shear Stress. ! Allowable Stress. ! Design of Simple Connections STRESS! Stress Evisdom! verage Normal Stress in an xially Loaded ar! verage Shear Stress! llowable Stress! Design of Simple onnections 1 Equilibrium of a Deformable ody ody Force w F R x w(s). D s y Support

More information

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection Mechanics of Materials II Chapter III A review of the fundamental formulation of stress, strain, and deflection Outline Introduction Assumtions and limitations Axial loading Torsion of circular shafts

More information

Theory at a Glance (for IES, GATE, PSU)

Theory at a Glance (for IES, GATE, PSU) 1. Stress and Strain Theory at a Glance (for IES, GATE, PSU) 1.1 Stress () When a material is subjected to an external force, a resisting force is set up within the component. The internal resistance force

More information

The science of elasticity

The science of elasticity The science of elasticity In 1676 Hooke realized that 1.Every kind of solid changes shape when a mechanical force acts on it. 2.It is this change of shape which enables the solid to supply the reaction

More information

9 MECHANICAL PROPERTIES OF SOLIDS

9 MECHANICAL PROPERTIES OF SOLIDS 9 MECHANICAL PROPERTIES OF SOLIDS Deforming force Deforming force is the force which changes the shape or size of a body. Restoring force Restoring force is the internal force developed inside the body

More information

Chapter 7. Highlights:

Chapter 7. Highlights: Chapter 7 Highlights: 1. Understand the basic concepts of engineering stress and strain, yield strength, tensile strength, Young's(elastic) modulus, ductility, toughness, resilience, true stress and true

More information

RODS: STATICALLY INDETERMINATE MEMBERS

RODS: STATICALLY INDETERMINATE MEMBERS RODS: STTICLLY INDETERMINTE MEMERS Statically Indeterminate ackground In all of the problems discussed so far, it was possible to determine the forces and stresses in the members by utilizing the equations

More information

High Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there?

High Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there? High Tech High Top Hat Technicians An Introduction to Solid Mechanics Or Is that supposed to bend there? Why don't we fall through the floor? The power of any Spring is in the same proportion with the

More information

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia):

Statics Principles. The laws of motion describe the interaction of forces acting on a body. Newton s First Law of Motion (law of inertia): Unit 2 Review Statics Statics Principles The laws of motion describe the interaction of forces acting on a body Newton s First Law of Motion (law of inertia): An object in a state of rest or uniform motion

More information

MECE 3321 MECHANICS OF SOLIDS CHAPTER 1

MECE 3321 MECHANICS OF SOLIDS CHAPTER 1 MECE 3321 MECHANICS O SOLIDS CHAPTER 1 Samantha Ramirez, MSE WHAT IS MECHANICS O MATERIALS? Rigid Bodies Statics Dynamics Mechanics Deformable Bodies Solids/Mech. Of Materials luids 1 WHAT IS MECHANICS

More information

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture five mechanics www.carttalk.com of materials Mechanics of Materials 1 Mechanics of Materials MECHANICS MATERIALS

More information

ME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft.

ME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft. ME 323 - Final Exam Name December 15, 2015 Instructor (circle) PROEM NO. 4 Part A (2 points max.) Krousgrill 11:30AM-12:20PM Ghosh 2:30-3:20PM Gonzalez 12:30-1:20PM Zhao 4:30-5:20PM M (x) y 20 kip ft 0.2

More information

Chapter 1 Introduction- Concept of Stress

Chapter 1 Introduction- Concept of Stress hapter 1 Introduction- oncept of Stress INTRODUTION Review of Statics xial Stress earing Stress Torsional Stress 14 6 ending Stress W W L Introduction 1-1 Shear Stress W W Stress and Strain L y y τ xy

More information

Aluminum shell. Brass core. 40 in

Aluminum shell. Brass core. 40 in PROBLEM #1 (22 points) A solid brass core is connected to a hollow rod made of aluminum. Both are attached at each end to a rigid plate as shown in Fig. 1. The moduli of aluminum and brass are EA=11,000

More information

N = Shear stress / Shear strain

N = Shear stress / Shear strain UNIT - I 1. What is meant by factor of safety? [A/M-15] It is the ratio between ultimate stress to the working stress. Factor of safety = Ultimate stress Permissible stress 2. Define Resilience. [A/M-15]

More information

ENG1001 Engineering Design 1

ENG1001 Engineering Design 1 ENG1001 Engineering Design 1 Structure & Loads Determine forces that act on structures causing it to deform, bend, and stretch Forces push/pull on objects Structures are loaded by: > Dead loads permanent

More information

CHAPTER 6 MECHANICAL PROPERTIES OF METALS PROBLEM SOLUTIONS

CHAPTER 6 MECHANICAL PROPERTIES OF METALS PROBLEM SOLUTIONS CHAPTER 6 MECHANICAL PROPERTIES OF METALS PROBLEM SOLUTIONS Concepts of Stress and Strain 6.1 Using mechanics of materials principles (i.e., equations of mechanical equilibrium applied to a free-body diagram),

More information

CHAPTER 4: BENDING OF BEAMS

CHAPTER 4: BENDING OF BEAMS (74) CHAPTER 4: BENDING OF BEAMS This chapter will be devoted to the analysis of prismatic members subjected to equal and opposite couples M and M' acting in the same longitudinal plane. Such members are

More information

Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3

Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3 Statics Chapter II Fall 2018 Exercises Corresponding to Sections 2.1, 2.2, and 2.3 2 3 Determine the magnitude of the resultant force FR = F1 + F2 and its direction, measured counterclockwise from the

More information

By Dr. Mohammed Ramidh

By Dr. Mohammed Ramidh Engineering Materials Design Lecture.6 the design of beams By Dr. Mohammed Ramidh 6.1 INTRODUCTION Finding the shear forces and bending moments is an essential step in the design of any beam. we usually

More information

March 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE

March 24, Chapter 4. Deflection and Stiffness. Dr. Mohammad Suliman Abuhaiba, PE Chapter 4 Deflection and Stiffness 1 2 Chapter Outline Spring Rates Tension, Compression, and Torsion Deflection Due to Bending Beam Deflection Methods Beam Deflections by Superposition Strain Energy Castigliano

More information

Twinning Engineering Programmes (TEP) & Thammasat English Programme of Engineering (TEPE) Faculty of Engineering, Thammasat University

Twinning Engineering Programmes (TEP) & Thammasat English Programme of Engineering (TEPE) Faculty of Engineering, Thammasat University " Twinning Engineering Programmes (TEP) & Thammasat English Programme of Engineering (TEPE) Faculty of Engineering, Thammasat University Undergraduate Examination 2 nd Semester of 2019 (Mid-term) CE221:

More information

STRESS, STRAIN AND DEFORMATION OF SOLIDS

STRESS, STRAIN AND DEFORMATION OF SOLIDS VELAMMAL COLLEGE OF ENGINEERING AND TECHNOLOGY, MADURAI 625009 DEPARTMENT OF CIVIL ENGINEERING CE8301 STRENGTH OF MATERIALS I -------------------------------------------------------------------------------------------------------------------------------

More information

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A (2 Marks) 1. Define longitudinal strain and lateral strain. 2. State Hooke s law. 3. Define modular ratio,

More information

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points)

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points) ME 270 3 rd Sample inal Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points) IND: In your own words, please state Newton s Laws: 1 st Law = 2 nd Law = 3 rd Law = PROBLEM

More information

Lecture 8 Viscoelasticity and Deformation

Lecture 8 Viscoelasticity and Deformation Read: pg 130 168 (rest of Chpt. 4) 1 Poisson s Ratio, µ (pg. 115) Ratio of the strain in the direction perpendicular to the applied force to the strain in the direction of the applied force. For uniaxial

More information

R13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A

R13. II B. Tech I Semester Regular Examinations, Jan MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) PART-A SET - 1 II B. Tech I Semester Regular Examinations, Jan - 2015 MECHANICS OF SOLIDS (Com. to ME, AME, AE, MTE) Time: 3 hours Max. Marks: 70 Note: 1. Question Paper consists of two parts (Part-A and Part-B)

More information

How materials work. Compression Tension Bending Torsion

How materials work. Compression Tension Bending Torsion Materials How materials work Compression Tension Bending Torsion Elemental material atoms: A. Composition a) Nucleus: protons (+), neutrons (0) b) Electrons (-) B. Neutral charge, i.e., # electrons = #

More information

5. What is the moment of inertia about the x - x axis of the rectangular beam shown?

5. What is the moment of inertia about the x - x axis of the rectangular beam shown? 1 of 5 Continuing Education Course #274 What Every Engineer Should Know About Structures Part D - Bending Strength Of Materials NOTE: The following question was revised on 15 August 2018 1. The moment

More information

Downloaded from Downloaded from / 1

Downloaded from   Downloaded from   / 1 PURWANCHAL UNIVERSITY III SEMESTER FINAL EXAMINATION-2002 LEVEL : B. E. (Civil) SUBJECT: BEG256CI, Strength of Material Full Marks: 80 TIME: 03:00 hrs Pass marks: 32 Candidates are required to give their

More information

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV UNIT I STRESS, STRAIN DEFORMATION OF SOLIDS PART A (2 MARKS)

More information

Strength of Material. Shear Strain. Dr. Attaullah Shah

Strength of Material. Shear Strain. Dr. Attaullah Shah Strength of Material Shear Strain Dr. Attaullah Shah Shear Strain TRIAXIAL DEFORMATION Poisson's Ratio Relationship Between E, G, and ν BIAXIAL DEFORMATION Bulk Modulus of Elasticity or Modulus of Volume

More information

PERIYAR CENTENARY POLYTECHNIC COLLEGE PERIYAR NAGAR - VALLAM THANJAVUR. DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK

PERIYAR CENTENARY POLYTECHNIC COLLEGE PERIYAR NAGAR - VALLAM THANJAVUR. DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK PERIYAR CENTENARY POLYTECHNIC COLLEGE PERIYAR NAGAR - VALLAM - 613 403 - THANJAVUR. DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK Sub : Strength of Materials Year / Sem: II / III Sub Code : MEB 310

More information

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. D : SOLID MECHANICS Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown. Q.2 Consider the forces of magnitude F acting on the sides of the regular hexagon having

More information

Chapter Two: Mechanical Properties of materials

Chapter Two: Mechanical Properties of materials Chapter Two: Mechanical Properties of materials Time : 16 Hours An important consideration in the choice of a material is the way it behave when subjected to force. The mechanical properties of a material

More information

Direct and Shear Stress

Direct and Shear Stress Direct and Shear Stress 1 Direct & Shear Stress When a body is pulled by a tensile force or crushed by a compressive force, the loading is said to be direct. Direct stresses are also found to arise when

More information

Laboratory 4 Bending Test of Materials

Laboratory 4 Bending Test of Materials Department of Materials and Metallurgical Engineering Bangladesh University of Engineering Technology, Dhaka MME 222 Materials Testing Sessional.50 Credits Laboratory 4 Bending Test of Materials. Objective

More information

SOLUTION 8 7. To hold lever: a+ M O = 0; F B (0.15) - 5 = 0; F B = N. Require = N N B = N 0.3. Lever,

SOLUTION 8 7. To hold lever: a+ M O = 0; F B (0.15) - 5 = 0; F B = N. Require = N N B = N 0.3. Lever, 8 3. If the coefficient of static friction at is m s = 0.4 and the collar at is smooth so it only exerts a horizontal force on the pipe, determine the minimum distance x so that the bracket can support

More information

Chapter 26 Elastic Properties of Materials

Chapter 26 Elastic Properties of Materials Chapter 26 Elastic Properties of Materials 26.1 Introduction... 1 26.2 Stress and Strain in Tension and Compression... 2 26.3 Shear Stress and Strain... 4 Example 26.1: Stretched wire... 5 26.4 Elastic

More information

Three torques act on the shaft. Determine the internal torque at points A, B, C, and D.

Three torques act on the shaft. Determine the internal torque at points A, B, C, and D. ... 7. Three torques act on the shaft. Determine the internal torque at points,, C, and D. Given: M 1 M M 3 300 Nm 400 Nm 00 Nm Solution: Section : x = 0; T M 1 M M 3 0 T M 1 M M 3 T 100.00 Nm Section

More information

Chapter 5 CENTRIC TENSION OR COMPRESSION ( AXIAL LOADING )

Chapter 5 CENTRIC TENSION OR COMPRESSION ( AXIAL LOADING ) Chapter 5 CENTRIC TENSION OR COMPRESSION ( AXIAL LOADING ) 5.1 DEFINITION A construction member is subjected to centric (axial) tension or compression if in any cross section the single distinct stress

More information

2012 MECHANICS OF SOLIDS

2012 MECHANICS OF SOLIDS R10 SET - 1 II B.Tech II Semester, Regular Examinations, April 2012 MECHANICS OF SOLIDS (Com. to ME, AME, MM) Time: 3 hours Max. Marks: 75 Answer any FIVE Questions All Questions carry Equal Marks ~~~~~~~~~~~~~~~~~~~~~~

More information

122 CHAPTER 2 Axially Loaded Numbers. Stresses on Inclined Sections

122 CHAPTER 2 Axially Loaded Numbers. Stresses on Inclined Sections 1 CHATER Aiall Loaded Numbers Stresses on Inclined Sections roblem.6-1 A steel bar of rectangular cross section (1.5 in..0 in.) carries a tensile load (see figure). The allowable stresses in tension and

More information

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS

Name :. Roll No. :... Invigilator s Signature :.. CS/B.TECH (CE-NEW)/SEM-3/CE-301/ SOLID MECHANICS Name :. Roll No. :..... Invigilator s Signature :.. 2011 SOLID MECHANICS Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are required to give their answers

More information

UNIT I SIMPLE STRESSES AND STRAINS

UNIT I SIMPLE STRESSES AND STRAINS Subject with Code : SM-1(15A01303) Year & Sem: II-B.Tech & I-Sem SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) UNIT I SIMPLE STRESSES

More information

PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics

PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics Page1 PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [2910601] Introduction, Fundamentals of Statics 1. Differentiate between Scalar and Vector quantity. Write S.I.

More information

MATERIALS. Why do things break? Why are some materials stronger than others? Why is steel tough? Why is glass brittle?

MATERIALS. Why do things break? Why are some materials stronger than others? Why is steel tough? Why is glass brittle? MATERIALS Why do things break? Why are some materials stronger than others? Why is steel tough? Why is glass brittle? What is toughness? strength? brittleness? Elemental material atoms: A. Composition

More information

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam. NAME: ME 270 Fall 2012 Examination No. 3 - Makeup Please review the following statement: Group No.: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

More information