2.1 When an axial load is applied to the ends of the bar shown in Fig. P2.1, the total elongation of the bar between joints A and C is 0.15 in. In segment (2), the normal strain is measured as 1,300 in./in. Determine: (a) the elongation of segment (2). (b) the normal strain in segment (1) of the bar. Fig. P2.1 Solution (a) From the definition of normal strain, the elongation in segment (2) can be computed as (1,300 10 6 )(90 in.) 0.1170 in. 2 2 L2 Ans. (b) The combined elongations of segments (1) and (2) is given as 0.15 in. Therefore, the elongation that occurs in segment (1) must be 0.15 in. 0.1170 in. 0.0330 in. 1 total 2 The strain in segment (1) can now be computed: 0.0330 in. 1 0.000825 in./in. 825 μin./in. 1 L1 40 in. Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.4 A rigid bar ABCD is supported by two bars as shown in Fig. P2.4. There is no strain in the vertical bars before load P is applied. After load P is applied, the normal strain in rod (1) is −570 m/m. Determine: (a) the normal strain in rod (2). (b) the normal strain in rod (2) if there is a 1-mm gap in the connection at pin C before the load is applied. (c) the normal strain in rod (2) if there is a 1-mm gap in the connection at pin B before the load is applied. Fig. P2.4 Solution (a) From the strain given for rod (1) 1 1 L1 ( 570 10 6 )(900 mm) 0.5130 mm Therefore, vB = 0.5130 mm (downward). From the deformation diagram of rigid bar ABCD vB vC 240 mm (240 mm 360 mm) 600 mm vC (0.5130 mm) 1.2825 mm 240 mm Therefore, 2 2 2 L2 = 1.2825 mm (elongation), and thus, from the definition of strain: 1.2825 mm 855 10 6 mm/mm 855 με 1,500 mm Ans. (b) The 1-mm gap at C doesn’t affect rod (1); therefore, 1 = −0.5130 mm. The rigid bar deformation diagram is unaffected; thus, vB = 0.5130 mm (downward) and vC = 1.2825 mm (downward). The rigid bar must move downward 1 mm at C before it begins to elongate member (2). Therefore, the elongation of member (2) is vC 1 mm 2 1.2825 mm 1 mm 0.2825 mm Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. and so the strain in member (2) is 0.2825 mm 2 188.3 10 2 L2 1,500 mm 6 mm/mm 188.3 με Ans. (c) From the strain given for rod (1), 1 = −0.5130 mm. In order to contract rod (1) by this amount, the rigid bar must move downward at B by vB 0.5130 mm 1 mm 1.5130 mm From deformation diagram of rigid bar ABCD vB vC 240 mm (240 mm 360 mm) 600 mm vC (1.5130 mm) 3.7825 mm 240 mm and so 3.7825 mm 2 2,521.7 10 6 mm/mm 2 L2 1,500 mm 2,520 με Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.8 A steel cable is used to support an elevator cage at the bottom of a 2,000-ft deep mineshaft. A uniform normal strain of 250 in./in. is produced in the cable by the weight of the cage. At each point, the weight of the cable produces an additional normal strain that is proportional to the length of the cable below the point. If the total normal strain in the cable at the cable drum (upper end of the cable) is 700 in./in., determine (a) the strain in the cable at a depth of 500 ft. (b) the total elongation of the cable. Solution Call the vertical coordinate y and establish the origin of the y axis at the lower end of the steel cable. The strain in the cable has a constant term (i.e., = 250 ) and a term (we will call it k) that varies with the vertical coordinate y. 250 10 6 k y The problem states that the normal strain at the cable drum (i.e., y = 2,000 ft) is 700 in./in. Knowing this value, the constant k can be determined 700 10 6 250 10 6 k (2, 000 ft) 700 10 6 250 10 6 0.225 10 6 /ft 2, 000 ft Substituting this value for k in the strain expression gives 250 10 6 (0.225 10 6 /ft) y k (a) At a depth of 500 ft, the y coordinate is y = 1,500 ft. Therefore, the cable strain at a depth of 500 ft is Ans. 250 10 6 (0.225 10 6 /ft)(1,500 ft) 587.5 10 6 588 με (b) The total elongation is found by integrating the strain expression over the cable length; thus, 2000 dy 250 10 6 (0.225 10 6 /ft) y dy 0 6 (250 10 ) y 0.225 10 2 0.950 ft 11.40 in. 2000 6 y 2 0 Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.9 The 16 × 22 × 25-mm rubber blocks shown in Fig. P2.9 are used in a double U shear mount to isolate the vibration of a machine from its supports. An applied load of P = 690 N causes the upper frame to be deflected downward by 7 mm. Determine the average shear strain and the shear stress in the rubber blocks. Fig. P2.9 Solution Consider the deformation of one block. After a downward deflection of 7 mm: 7 mm tan 0.4375 0.412410 rad 16 mm and thus, the shear strain in the block is Ans. 0.412 rad 412,000 μrad Note that the small angle approximation most definitely does not apply here! The applied load of 690 N is carried by two blocks; therefore, the shear force applied to one block is V = 345 N. The area subjected to shear stress is the area that is parallel to the direction of the shear force; that is, the 22 mm by 25 mm surface of the block. The shear stress is 345 N (22 mm)(25 mm) 0.627 MPa 627 kPa Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.12 A thin rectangular plate is uniformly deformed as shown in Fig. P2.12. Determine the shear strain xy at P. Fig. P2.12 Solution Before deformation, the angle of the plate at P was 90° or /2 radians. We must now determine the plate angle at P after deformation. The difference between these angles is the shear strain. After deformation, the angle that side PQ makes with the horizontal axis is 1.4 mm tan 1,100 mm 0.072922 and the angle that side PR makes with the vertical axis is 0.7 mm tan 600 mm 0.066845 Therefore, the angle of the plate at P that was initially 90° has been reduced by the sum of and : 0.072922 0.066845 0.139767 0.002439 rad Since shear strain is defined as the change in angle between two initially perpendicular lines, the shear strain in the plate at P is Ans. 0.002439 rad 2,440 μrad P Note: Since these angles are small, we could have just as well used tan ≈ and tan the extra steps involved in using the inverse tangent function. Thus, 1.4 mm tan 0.001273 rad 1,100 mm 0.7 mm tan 0.001167 rad 600 mm 0.001273 rad 0.001167 rad 0.002439 rad 2,440 μrad P ≈ and saved Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.18 At a temperature of 40°F, a 0.08-in. gap exists between the ends of the two bars shown in Fig. P2.18. Bar (1) is an aluminum alloy [ = 12.5 × 10−6/°F] and bar (2) is stainless steel [ = 9.6 × 10−6/°F]. The supports at A and C are rigid. Determine the lowest temperature at which the two bars contact each other. Fig. P2.18 Solution Write expressions for the temperature-induced deformations and set this equal to the 0.08-in. gap: 0.08 in. 1 T L1 2 T L2 T L 1 1 2 L2 0.08 in. 0.08 in. 0.08 in. 77.821°F -6 (12.5 10 / °F)(40 in.) (9.6 10-6 / °F)(55 in.) 1 L1 2 L2 Since the initial temperature is 40°F, the temperature at which the gap is closed is 117.8°F. T Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. 2.21 Determine the movement of the pointer of Fig. P2.21 with respect to the scale zero in response to a temperature increase of 60°F. The coefficients of thermal expansion are 6.6×10-6/°F for the steel and 12.5×10-6/°F for the aluminum. Fig. P2.21 Solution In response to the 60°F temperature increase, the steel pieces elongate by the amount (6.6 10 6 /°F)(60°F)(12 in.) 0.004752 in. Steel Steel T LSteel and the aluminum piece elongates by (12.5 10 6 /°F)(60°F)(12 in.) 0.009000 in. Alum Alum T LAlum From the deformation diagram of the pointer, the scale reading can be determined from similar triangles vpointer Alum Steel 1.5 in. vpointer 8.5 in. 8.5 in. Alum 1.5 in. Steel 5.6667 0.009000 in. 0.004752 in. 0.0241 in. (upward) Ans. Excerpts from this work may be reproduced by instructors for distribution on a not-for-profit basis for testing or instructional purposes only to students enrolled in courses for which the textbook has been adopted. Any other reproduction or translation of this work beyond that permitted by Sections 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful.