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05-01ChapGere

Course: EM em319, Spring 2008
School: University of Texas
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in 5 Stresses Beams (Basic Topics) Longitudinal Strains in Beams Problem 5.4-1 Determine the maximum normal strain max produced in a steel wire of diameter d 1/16 in. when it is bent around a cylindrical drum of radius R 24 in. (see figure). d R Solution 5.4-1 Steel wire R 24 in. d 1 in. 16 R Cylinder d From Eq. (5-4): y emax r d2 d R d 2 2R d Substitute numerical values: emax 1 16 in. 2(24 in.) 1 16 in....

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in 5 Stresses Beams (Basic Topics) Longitudinal Strains in Beams Problem 5.4-1 Determine the maximum normal strain max produced in a steel wire of diameter d 1/16 in. when it is bent around a cylindrical drum of radius R 24 in. (see figure). d R Solution 5.4-1 Steel wire R 24 in. d 1 in. 16 R Cylinder d From Eq. (5-4): y emax r d2 d R d 2 2R d Substitute numerical values: emax 1 16 in. 2(24 in.) 1 16 in. 1300 10 6 Problem 5.4-2 A copper wire having diameter d 3 mm is bent into a circle and held with the ends just touching (see figure). If the maximum permissible strain in the copper is max 0.0024, what is the shortest length L of wire that can be used? d = diameter L = length Solution 5.4-2 Copper wire d d L 3 mm 2 r r max 0.0024 L 2 d L (3 mm) 0.0024 3.93 m From Eq. (5-4): emax L min y r d emax d2 L2 285 286 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.4-3 A 4.5 in. outside diameter polyethylene pipe designed to carry chemical wastes is placed in a trench and bent around a quartercircular 90 bend (see figure). The bent section of the pipe is 46 ft long. Determine the maximum compressive strain max in the pipe. 90 Solution 5.4-3 Polyethylene pipe d Angle equals 90 or /2 radians, r radius of curvature L L d L length of 90 bend 46 ft 552 in. 4.5 in. 2 r 4 r 2 emax r L 2 d 4L 2L emax y r d2 2L 6400 10 6 L r r radius 4.5 in. 4 552 in. Problem 5.4-4 A cantilever beam AB is loaded by a couple M0 at its free end (see figure). The length of the beam is L 1.5 m and the longitudinal normal strain at the top surface is 0.001. The distance from the top surface of the beam to the neutral surface is 75 mm. Calculate the radius of curvature , the curvature , and the vertical deflection at the end of the beam. Solution 5.4-4 Cantilever beam L A C B M0 A B L M0 Assume that the deflection curve is nearly flat. Then the distance BC is the same as the length L of the beam. sin u L r 1.5 m 75 m 0.02 0 length of beam 1.5 m 0.001 max y y 75 mm emax r y 75 mm r 75 m emax 0.001 1 k 0.01333 m 1 r L L arcsin 0.02 0.02 rad (1 cos ) (75 m)(1 cos (0.02 rad)) 15.0 mm L NOTE: 100, which confirms that the deflection curve is nearly flat. SECTION 5.4 Longitudinal Strains in Beams 287 Problem 5.4-5 A thin strip of steel of length L 20 in. and thickness t 0.2 in. is bent by couples M0 (see figure). The deflection at the midpoint of the strip (measured from a line joining its end points) is found to be 0.25 in. Determine the longitudinal normal strain at the top surface of the strip. M0 M0 t L -- 2 L -- 2 Solution 5.4-5 Thin strip of steel 0 The deflection curve is very flat (note that L/ and therefore is a very small angle. sin u L2 r sin u (1 L2 ( is in radians) r cos ) 80) For small angles, u M0 M0 L -- 2 L -- 2 Substitute numerical values ( 0.25 r 1 cos 10 r r 1 cos cos L 2r inches): L 20 in. t 0.25 in. 0.2 in. Solve numerically: 200.0 in. NORMAL STRAIN y t 2 0.1 in. e r r 200 in. 500 10 6 (Shortening at the top surface) Problem 5.4-6 A bar of rectangular cross section is loaded and supported as shown in the figure. The distance between supports is L 1.2 m and the height of the bar is h 100 mm. The deflection at the midpoint is measured as 3.6 mm. What is the maximum normal strain at the top and bottom of the bar? h P P a L -- 2 L -- 2 a 288 CHAPTER 5 Stresses in Beams (Basic Topics) Solution 5.4-6 Bar of rectangular cross section h P P a L -- 2 L -- 2 a 0 L 1.2 m h 100 mm 3.6 mm Substitute numerical values ( 0.0036 r 1 cos 0.6 r meters): Note that the deflection curve is nearly flat (L/ 333) and is a very small angle. sin u u L2 r Solve numerically: NORMAL STRAIN r 1 L cos 2r e y r h2 r 50.00 m L2 (radians) r r (1 cos u) 50 mm 50,000 mm 1000 10 6 (Elongation on top; shortening on bottom) Normal Stresses in Beams Problem 5.5-1 A thin strip of hard copper (E 16,400 ksi) having length L 80 in. and thickness t 3/32 in. is bent into a circle and held with the ends just touching (see figure). (a) Calculate the maximum bending stress max in the strip. (b) Does the stress increase or decrease if the thickness of the strip is increased? 3 t = -- in. 32 Solution 5.5-1 E 16,400 ksi Copper strip bent into a circle L 80 in. t 3/32 in. Substitute numerical values: smax (16,400 ksi)(3 32 in.) 80 in. 60.4 ksi (a) MAXIMUM BENDING STRESS L 2 r 2 r r L 2 Ey r Et L 2 Ey L (b) CHANGE IN STRESS If the thickness t is increased, the stress max From Eq. (5-7): s smax 2 E(t 2) L increases. SECTION 5.5 Normal Stresses in Beams 289 Problem 5.5-2 A steel wire (E 200 GPa) of diameter d 1.0 mm is bent around a pulley of radius R0 400 mm (see figure). (a) What is the maximum stress max in the wire? (b) Does the stress increase or decrease if the radius of the pulley is increased? R0 d Solution 5.5-2 E 200 GPa Steel wire bent around a pulley d 1.0 mm R0 400 mm From Eq. (5-7): smax 400.5 mm Ey r (200 GPa) (0.5 mm) 400.5 mm 250 MPa (a) MAXIMUM STRESS IN THE WIRE r y R0 d 2 d 2 400 mm 0.5 mm (b) CHANGE IN STRESS If the radius is increased, the stress decreases. max 0.5 mm Problem 5.5-3 A thin, high-strength steel rule (E 30 106 psi) having thickness t 0.15 in. and length L 40 in. is bent by couples M0 into a circular arc subtending a central angle 45 (see figure). (a) What is the maximum bending stress max in the rule? (b) Does the stress increase or decrease if the central angle is increased? L = length t M0 M0 Solution 5.5-3 L Thin steel rule bent into an arc Substitute numerical values: smax E t L 30 106 psi 0.15 in. 40 in. 45 0.78540 rad (30 106 psi) (0.15 in.) (0.78540 rad) 2 (40 in.) 44,200 psi 44.2 ksi (b) CHANGE IN STRESS If the angle increases. is increased, the stress max (a) MAXIMUM BENDING STRESS L smax r Ey r r L E(t 2) L radians Et 2L 290 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-4 A simply supported wood beam AB with span length L 3.5 m carries a uniform load of intensity q 6.4 kN/m (see figure). Calculate the maximum bending stress max due to the load q if the beam has a rectangular cross section with width b 140 mm and height h 240 mm. q A B h L b Solution 5.5-4 L b Mmax smax Simple beam with uniform load Substitute numerical values: smax 3(6.4 kN m)(3.5 m) 2 4(140 mm)(240 mm) 2 7.29 MPa 3.5 m q 6.4 kN/m 140 mm h 240 mm qL 8 2 S bh 6 3qL2 4bh2 2 Mmax S Problem 5.5-5 Each girder of the lift bridge (see figure) is 180 ft long and simply supported at the ends. The design load for each girder is a uniform load of intensity 1.6 k/ft. The girders are fabricated by welding three steel plates so as to form an I-shaped cross section (see figure) having section modulus S 3600 in3. What is the maximum bending stress max in a girder due to the uniform load? Solution 5.5-5 Bridge girder q L S Mmax L 180 ft 3600 in.3 qL2 8 Mmax S q 1.6 k/ft smax smax qL2 8S 21.6 ksi (1.6 k ft)(180 ft) 2 (12 in. ft) 8(3600 in.3 ) SECTION 5.5 Normal Stresses in Beams 291 Problem 5.5-6 A freight-car axle AB is loaded approximately as shown in the figure, with the forces P representing the car loads (transmitted to the axle through the axle boxes) and the forces R representing the rail loads (transmitted to the axle through the wheels). The diameter of the axle is d 80 mm, the distance between centers of the rails is L, and the distance between the forces P and R is b 200 mm. Calculate the maximum bending stress max in the axle if P 47 kN. P A d R b L R P B d b Solution 5.5-6 Freight-car axle MAXIMUM BENDING STRESS smax Mmax S 32Pb d3 Diameter d 80 mm Distance b 200 mm Load P 47 kN M max Pb S d3 32 Substitute numerical values: smax 32(47 kN)(200 mm) (80 mm) 3 187 MPa Problem 5.5-7 A seesaw weighing 3 lb/ft of length is occupied by two children, each weighing 90 lb (see figure). The center of gravity of each child is 8 ft from the fulcrum. The board is 19 ft long, 8 in. wide, and 1.5 in. thick. What is the maximum bending stress in the board? Solution 5.5-7 Seesaw b q h b P q P 8 in. h 1.5 in. 3 lb/ft P 90 lb Pd qL2 2 d 8.0 ft 135.4 lb-ft L 9.5 ft Mmax 720 lb-ft 855.4 lb-ft 10,264 lb-in. d L d L bh2 3.0 in3. 6 M 10,264 lb-in. smax S 3.0 in.3 S 3420 psi 292 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-8 During construction of a highway bridge, the main girders are cantilevered outward from one pier toward the next (see figure). Each girder has a cantilever length of 46 m and an I-shaped cross section with dimensions as shown in the figure. The load on each girder (during construction) is assumed to be 11.0 kN/m, which includes the weight of the girder. Determine the maximum bending stress in a girder due to this load. 50 mm 2400 mm 25 mm 600 mm Solution 5.5-8 Bridge girder Mmax qL2 2 Mmax c I b1h3 1 12 1 (11.0 kN m)(46 m) 2 2 c h 2 1200 mm 11,638 kN m q tf smax h1 tw L h2 I bh3 12 b 1 1 (0.6 m)(2.4 m) 3 (0.575 m)(2.3 m) 3 12 12 0.6912 m4 0.5830 m4 0.1082 m4 smax Mmax c I (11,638 kN m)(1.2 m) 0.1082 m4 129 MPa L q b tf h1 b1 46 m 11.0 kN/m 600 mm h 2400 mm 50 mm tw 25 mm h 2tf 2300 mm b tw 575 mm Problem 5.5-9 The horizontal beam ABC of an oil-well pump has the cross section shown in the figure. If the vertical pumping force acting at end C is 8.8 k, and if the distance from the line of action of that force to point B is 14 ft, what is the maximum bending stress in the beam due to the pumping force? A B C 0.875 in. 0.625 in. 20.0 in. 8.0 in. SECTION 5.5 Normal Stresses in Beams 293 Solution 5.5-9 Beam in an oil-well pump Mmax tf PL (8.8 k)(14 ft) 123,200 lb-ft 1,478,400 lb-in. Mmax c I b1h3 1 12 1 (7.375 in.)(18.25 in.) 3 12 1,597.7 in.4 c h 2 10.0 in. smax P L h1 tw h2 I bh3 12 b 1 (8.0 in.)(20.0 in.) 3 12 5,333.3 in.4 3,735.7 in.4 (1.4784 L P b tf h1 b1 14 ft 8.8 k 8.0 in. h 20.0 in. 0.875 in. tw 0.625 in. h 2tf 18.25 in. b tw 7.375 in. smax Mmax c I 106 lb-in.)(10.0 in.) 1,597.7 in.4 9.25 ksi 9250 psi Problem 5.5-10 A railroad tie (or sleeper) is subjected to two rail loads, each of magnitude P 175 kN, acting as shown in the figure. The reaction q of the ballast is assumed to be uniformly distributed over the length of the tie, which has cross-sectional dimensions b 300 mm and h 250 mm. Calculate the maximum bending stress max in the tie due to the loads P, assuming the distance L 1500 mm and the overhang length a 500 mm. P a L P a b h q Solution 5.5-10 DATA P L q Railroad tie (or sleeper) 250 mm Substitute numerical values: M1 3 175 kN b 300 mm h 1500 mm a 500 mm 2P L 2a S bh2 6 3.125 10 17,500 N m 21,875 N m M2 21,875 N m m3 Mmax BENDING-MOMENT DIAGRAM M1 0 M2 M1 MAXIMUM BENDING STRESS smax Mmax 5 21,875 N m 3.125 10 3 m3 7.0 MPa (Tension on top; compression on bottom) M1 M2 q L 2 2 P qa2 2 Pa2 L 2a a 2 L P (2a 4 L 2a 2 L) a PL 2 2 PL 2 294 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-11 A fiberglass pipe is lifted by a sling, as shown in the figure. The outer diameter of the pipe is 6.0 in., its thickness is 0.25 in., and its weight density is 0.053 lb/in.3 The length of the pipe is L 36 ft and the distance between lifting points is s 11 ft. Determine the maximum bending stress in the pipe due to its own weight. s L Solution 5.5-11 Pipe lifted by a sling q t a s L a d1 d2 L s 36 ft 11 ft 432 in. 132 in. A d2 d1 4 6.0 in. d2 2t (d 2 2 d 2) 1 t 0.25 in. 5.5 in. 4.5160 in.2 I q (d 4 d 4 ) 18.699 in.4 1 64 2 A (0.053 lb/in.3)(4.5160 in.2) 0.23935 lb/in. 0.053 lb/in.3 a (L s)/2 150 in. BENDING-MOMENT DIAGRAM 0 M1 M2 M1 MAXIMUM BENDING STRESS smax smax Mmax c I c d2 2 3.0 in. 432 psi M1 M2 Mmax 2,692.7 lb-in. qa2 2 qL L 4 2 2,692.7 lb-in. s 2,171.4 lb-in. (2,692.7 lb-in.)(3.0 in.) 18.699 in.4 (Tension on top) SECTION 5.5 Normal Stresses in Beams 295 Problem A 5.5-12 small dam of height h 2.0 m is constructed of vertical wood beams AB of thickness t 120 mm, as shown in the figure. Consider the beams to be simply supported at the top and bottom. Determine the maximum bending stress max in the beams, assuming that the weight density of water is 9.81 kN/m3. h t A B Solution 5.5-12 Vertical wood beam t A A MAXIMUM BENDING MOMENT q0 q q0 ( x ) L B h RA x L RA B q0 q0 L 6 h t 2.0 m 120 mm 9.81 kN/m3 (water) Let b width of beam perpendicular to the plane of the figure Let q0 q0 gbh maximum intensity of distributed load S bt 6 2 q0 x3 6L q0 Lx q0 x3 6 6L dM q0L q0 x2 L 0 x dx 6 2L 3 Substitute x L 3 into the equation for M: M RAx Mmax For the vertical wood beam: L Maximum bending stress smax Mmax S 2q0 h2 q0 L L 6 3 q0 L3 6L 3 3 q0 L2 9 3 h; Mmax q0 h2 9 3 2gh3 3 3 t2 3 3 bt 2 SUBSTITUTE NUMERICAL VALUES: max 2.10 MPa NOTE: For b 1.0 m, we obtain q0 19,620 N/m, S 0.0024 m3, Mmax 5,034.5 N m, and Mmax/S 2.10 MPa max 296 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-13 Determine the maximum tensile stress t (due to pure bending by positive bending moments M) for beams having cross sections as follows (see figure): (a) a semicircle of diameter d, and (b) an isosceles trapezoid with bases b1 b and b2 4b/3, and altitude h. b1 C d (a) C b2 (b) h Solution 5.5-13 (a) SEMICIRCLE Maximum tensile stress (b) TRAPEZOID C c d c b2 b1 C h From Appendix D, Case 10: IC c st (9 4r 3 Mc IC 2 64)r4 (9 72 2d 3 768M (9 2 64)d3 64)d 4 1152 2 4b 3 From Appendix D, Case 8: b1 b b2 IC h3 (b2 4b1b2 b2 ) 1 2 36(b1 b2 ) 73bh3 756 c st h(2b1 b2 ) 3(b1 b2 ) Mc IC 360M 73bh2 10h 21 30.93 M d3 Problem 5.5-14 Determine the maximum bending stress max (due to pure bending by a moment M) for a beam having a cross section in the form of a circular core (see figure). The circle has diameter d and the angle 60. (Hint: Use the formulas given in Appendix D, Cases 9 and 15.) C d SECTION 5.5 Normal Stresses in Beams 297 Solution 5.5-14 Circular core From Appendix D, Cases 9 and 15: y C y Iy r d 2 r4 4 r4 2 ab r2 b d 2 a 2ab3 r4 MAXIMUM BENDING STRESS smax smax For smax Mc Iy 3 c r sin b d sin b 2 64M sin b d (4b sin 4b) 60 /3 rad: 3 radians Iy d 64 4 d4 64 d4 64 d4 64 d 32 2 4 radians b b b b r sin sin b cos b d4 32 2 d4 32 2 (sin b cos b)(1 2 sin b cos3 b 2 cos2b) b r cos 576M (8 3 9)d 10.96 M d3 d4 32 2 d4 (4b 128 sin 4b) 1 sin 4b 4 1 sin 2b ( cos 2b) 2 Problem 5.5-15 A simple beam AB of span length L 24 ft is subjected to two wheel loads acting at distance d 5 ft apart (see figure). Each wheel transmits a load P 3.0 k, and the carriage may occupy any position on the beam. Determine the maximum bending stress max due to the wheel loads if the beam is an I-beam having section modulus S 16.2 in.3 P d P C A B L Solution 5.5-15 P x A d Wheel loads on a beam P Substitute x into the equation for M: L d P S 24 ft 288 in. 5 ft 60 in. 3k 16.2 in.3 Mmax P L 2L d 2 2 B MAXIMUM BENDING STRESS smax Mmax S P L 2LS RA L MAXIMUM BENDING MOMENT RA M dM dx P (L L RAx x) P (L L dx 4x) x d) P (2L L d 2x) Substitute numerical values: smax d 2 2 30 in.) 2 3k (288 in. 2(288 in.)(16.2 in.3 ) 21.4 ksi P (2Lx L d 2x2 ) 0 x L 2 d 4 P (2L L 298 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-16 Determine the maximum tensile stress t and maximum compressive stress c due to the load P acting on the simple beam AB (see figure). Data are as follows: P 5.4 kN, L 3.0 m, d 1.2 m, b 75 mm, t 25 mm, h 100 mm, and h1 75 mm. t P A d B h h1 L b Solution 5.5-16 Simple beam of T-section t P A d B c2 RA L RB b c1 C h1 h P b d 5.4 kN 75 mm 1.2 m L t h 3.0 m 25 mm 100 mm h1 75 mm MAXIMUM BENDING MOMENT Mmax RA(L d) RB(d) 3888 N m MAXIMUM TENSILE STRESS st Mmax c2 IC 43.9 MPa MAXIMUM COMPRESSIVE STRESS sc Mmax c1 IC 73.2 MPa (3888 N m)(0.0625 m) 3.3203 106 mm4 PROPERTIES OF THE CROSS SECTION A c1 IC 3750 mm2 c2 37.5 mm (3888 N m)(0.0375 m) 3.3203 106 mm4 62.5 mm 3.3203 106 mm4 REACTIONS OF THE BEAM RA 2.16 kN RB 3.24 kN Problem 5.5-17 A cantilever beam AB, loaded by a uniform load and a concentrated load (see figure), is constructed of a channel section. Find the maximum tensile stress t and maximum compressive stress c if the cross section has the dimensions indicated and the moment of inertia about the z axis (the neutral axis) is I 2.81 in.4 (Note: The uniform load represents the weight of the beam.) 200 lb 20 lb/ft B 5.0 ft y z C 3.0 ft A 0.606 in. 2.133 in. SECTION 5.5 Normal Stresses in Beams 299 Solution 5.5-17 Cantilever beam (channel section) 200 lb I 2.81 in.4 c1 0.606 in. 20 lb/ft B 5.0 ft Mmax (200 lb)(5.0 ft) A 3.0 ft 8.0 ft 1000 lb-ft 640 lb-ft 19,680 lb-in. (20 lb ft)(8.0 ft) 1640 lb-ft c2 2.133 in. 8.0 ft 2 y z C 0.606 in. 2.133 in. MAXIMUM TENSILE STRESS Mc1 (19,680 lb-in.)(0.606 in.) st I 2.81 in.4 4,240 psi MAXIMUM COMPRESSIVE STRESS sc Mc2 I (19,680 lb-in.)(2.133 in.) 2.81 in.4 14,940 psi Problem 5.5-18 A cantilever beam AB of triangular cross section has length L 0.8 m, width b 80 mm, and height h 120 mm (see figure). The beam is made of brass weighing 85 kN/m3. (a) Determine the maximum tensile stress t and maximum compressive stress c due to the beam's own weight. (b) If the width b is doubled, what happens to the stresses? (c) If the height h is doubled, what happens to the stresses? A B b h L Solution 5.5-18 Triangular beam q y b z L h/3 2h h 3 C L 0.8 m b 85 kN/m3 g bh 2 80 mm h 120 mm Compressive stress: c 2 t t c Substitute numerical values: (a) MAXIMUM STRESSES q Iz gA IC Mmax h 3 Mc1 Iz c2 qL2 2 2h 3 3gL h 2 1.36 MPa 2.72 MPa gbhL2 4 (b) WIDTH b IS DOUBLED No change in stresses. (c) HEIGHT h IS DOUBLED Stresses are reduced by half. bh3 36 c1 Tensile stress: st 300 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-19 A beam ABC with an overhang from B to C supports a uniform load of 160 lb/ft throughout its length (see figure). The beam is a channel section with dimensions as shown in the figure. The moment of inertia about the z axis (the neutral axis) equals 5.14 in.4 Calculate the maximum tensile stress t and maximum compressive stress c due to the uniform load. 160 lb/ft A B 10 ft C 5 ft y z C 0.674 in. 2.496 in. Solution 5.5-19 Beam with an overhang q 160 lb/ft y 0.674 in. 2.496 in. A L 10 ft B b 5 ft C z C AT CROSS SECTION OF MAXIMUM POSITIVE M1 0 3.75 ft M2 BENDING MOMENT st sc M1c2 Iz M1c1 Iz (13,500 lb-in.)(2.496 in.) 5.14 in.4 (13,500 lb-in.)(0.674 in.) 5.14 in.4 6,560 psi 1,770 psi Iz c1 RA M1 M2 5.14 in.4 0.674 in. c2 2.496 in. 600 lb RB 1800 lb 1125 lb-ft 13,500 lb-in. 2000 lb-ft 24,000 lb-in. AT CROSS SECTION OF MAXIMUM NEGATIVE BENDING MOMENT st sc M2c1 Iz M2c2 Iz (24,000 lb-in.)(0.674 in.) 5.14 in.4 (24,000 lb-in.)(2.496 in.) 5.14 in.4 3,150 psi 11,650 psi MAXIMUM STRESSES 6,560 psi t c 11,650 psi Problem 5.5-20 A frame ABC travels horizontally with an acceleration a0 (see figure). Obtain a formula for the maximum stress max in the vertical arm AB, which has length L, thickness t, and mass density . L A t a0 = acceleration B C SECTION 5.5 Normal Stresses in Beamss 301 Solution 5.5-20 L t Accelerating frame TYPICAL UNITS FOR USE IN THE PRECEDING EQUATION length of vertical arm thickness of vertical arm mass density a0 acceleration Let b width of arm perpendicular to the plane of the figure Let q inertia force per unit distance along vertical arm VERTICAL ARM t SI UNITS: kg/m3 L meters (m) a0 t m/s2 meters (m) max N s2/m4 N/m2 (pascals) slug/ft3 ft/s2 t lb-s2/ft4 ft L q q rbta0 bt 2 6 Mmax smax qL2 2 Mmax S rbta0 L2 2 3rL2a0 t USCS UNITS: L max ft a0 S lb/ft2 (Divide by 144 to obtain psi) Problem 5.5-21 A beam of T-section is supported and loaded as shown in the figure. The cross section has width b 2 1/2 in., height h 3 in., and thickness t 1/2 in. Determine the maximum tensile and compressive stresses in the beam. P = 625 lb L1 = 4 ft q = 80 lb/ft 1 t = -- in. 2 t = -- in. 2 1 h= 3 in. L2 = 8 ft L3 = 5 ft b = 2 -- in. 2 1 Solution 5.5-21 P L1 A Beam of T-section q B C qL2 3 2 BENDING-MOMENT DIAGRAM M1 RA L1 9,000 lb in. L2 RA RB L3 BENDING MOMENT M2 12,000 lb in. AT CROSS SECTION OF MAXIMUM POSITIVE 5 ft 60 in. st M1c2 IC 4,320 psi sc M1c1 IC 8,640 psi L1 P 4 ft 48 in. L2 8 ft 96 in. L3 625 lb q 80 lb/ft 6.6667 lb/in. t c1 C h t b c2 PROPERTIES OF THE CROSS SECTION b 2.5 in. h 3.0 in. t 0.5 in. A bt (h t)t 2.50 in.2 c1 2.0 in. c2 1.0 in. IC 25 4 in. 12 2.0833 in.4 AT CROSS SECTION OF MAXIMUM NEGATIVE BENDING MOMENT st M2c1 IC 11,520 psi sc M2c2 IC 5,760 psi REACTIONS RA 187.5 lb (upward) RB 837.5 lb (upward) MAXIMUM STRESSES 11,520 psi t c 8,640 psi 302 CHAPTER 5 Stresses in Beams (Basic Topics) Problem 5.5-22 A cantilever beam AB with a rectangular cross section has a longitudinal hole drilled throughout its length (see figure). The beam supports a load P 600 N. The cross section is 25 mm wide and 50 mm high, and the hole has a diameter of 10 mm. Find the bending stresses at the top of the beam, at the top of the hole, and at the bottom of the beam. 10 mm A 50 mm B 12.5 mm P = 600 N L = 0.4 m 25 mm 37.5 mm Solution 5.5-22 Rectangular beam with a hole y c1 z c2 B C y B MOMENT OF INERTIA ABOUT THE NEUTRAL AXIS (THE z AXIS) All dimensions in millimeters. Rectangle: Iz Ic Ad 2 1 (25)(50) 3 (25)(50)(25 12 260,420 Hole: Iz Ic Ad 2 878 261,300 mm4 24.162) 2 24.162) 2 MAXIMUM BENDING MOMENT M PL (600 N)(0.4 m) 240 N m PROPERTIES OF THE CROSS SECTION A1 area of rectangle (25 mm)(50 mm) A2 area of hole (10 mm) 78.54 mm 4 area of cross section A1 A2 1171.5 mm2 2 2 1250 mm2 490.87 Cross-section: I 261,300 14,460 (10) 4 (78.54)(37.5 64 13,972 14,460 mm4 246,800 mm4 A STRESS AT THE TOP OF THE BEAM Mc1 (240 N m)(25.838 mm) s1 I 246,800 mm4 25.1 MPa (tension) STRESS AT THE TOP OF THE HOLE My s2 y c1 7.5 mm 18.338 mm I s2 (240 N m)(18.338 mm) 246,800 mm4 Using line B-B as reference axis: Ai yi y A1(25 mm) A2(37.5 mm) 28,305 mm3 3 a Ai yi 28,305 mm A 1171.5 mm2 Distances to the centroid C: 24.162 mm 17.8 MPa (tension) c2 c1 y 24.162 mm c2 25.838 mm 50 mm STRESS AT THE BOTTOM OF THE BEAM Mc2 (240 N m)(24.162 mm) s3 I 246,800 mm4 23.5 MPa (compression) SECTION 5.5 Normal Stresses in Beams 303 Problem 5.5-23 A small dam of height h 6 ft is constructed of vertical wood beams AB, as shown in the figure. The wood beams, which have thickness t 2.5 in., are simply supported by horizontal steel beams at A and B. Construct a graph showing the maximum bending stress max in the wood beams versus the depth d of the water above the lower support at B. Plot the stress max (psi) as the ordinate and the depth d (ft) as the abscissa. (Note: The weight density of water equals 62.4 lb/ft3.) Steel beam A Wood beam t h d B Steel beam t Wood beam Side view Top view Solution 5.5-23 A t Vertical wood beam in a dam 6 ft 2.5 in. 62.4 lb/ft3 Let b width of beam (perpendicular to the figure) Let q0 intensity of load at depth d q0 bd h t MAXIMUM BENDING STRESS 1 2 Section modulus: S bt 6 smax q0 smax Mmax S bd gd 3 1 t2 h d B q0 6 q0 d 2 B 1 6 bt 2 d L d L ANALYSIS OF BEAM q0 L RA A C B RB x0 MC RA L d RB h 6 ft q0 d 2 6L q0 d 3 6 d d B 3L RA (L d L d) q0 d 6 2 SUBSTITUTE NUMERICAL VALUES: d depth of water (ft) (Max. d h 6 ft) L h 6 ft 62.4 lb/ft3 t 2.5 in. psi max smax (62.4)d 3 1 (2.5) 2 d 6 9d d d 9B 18 d max 2d d 3LB 3L 2d d R 3LB 3L 0.1849d 3 (54 1 2d) V RA d L d (ft) 0 1 2 3 4 5 6 (psi) 0 C x0 RB 0 9 59 171 347 573 830 M Mmax MC 1000 750 830 psi 0 max (psi) Mmax q0 d 2 1 6 d L 2d d 3LB 3L 500 250 0 1 2 3 d (ft) 4 5 6
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RPI - PHYS - 1200
1. The magnitude of the force of one particle on the other is given by F = Gm1m2/r2, where m1 and m2 are the masses, r is their separation, and G is the universal gravitational constant. We solve for r:Gm1m2 = r= F( 6.67 10-11N m 2 / kg 2 ) (
RPI - PHYS - 1200
1. The air inside pushes outward with a force given by piA, where pi is the pressure inside the room and A is the area of the window. Similarly, the air on the outside pushes inward with a force given by poA, where po is the pressure outside. The mag
RPI - PHYS - 1200
1. (a) The amplitude is half the range of the displacement, or xm = 1.0 mm. (b) The maximum speed vm is related to the amplitude xm by vm = xm, where is the angular frequency. Since = 2f, where f is the frequency,vm = 2 fxm = 2 (120 Hz ) (1.0 10 -
RPI - PHYS - 1200
1. (a) The motion from maximum displacement to zero is one-fourth of a cycle so 0.170 s is one-fourth of a period. The period is T = 4(0.170 s) = 0.680 s. (b) The frequency is the reciprocal of the period:f = 1 1 = = 1.47 Hz. T 0.680 s(c) A sinuso
RPI - PHYS - 1200
1. The time it takes for a soldier in the rear end of the column to switch from the left to the right foot to stride forward is t = 1 min/120 = 1/120 min = 0.50 s. This is also the time for the sound of the music to reach from the musicians (who are
University of Texas - BIO - 325
23. How does a gene become a merozygote? The Hfr cell has an F factor integrated into its chromosome. The f factor (which is an episome because it can excise itself and integrate itself into the chromosomal DNA) excises itself sloppily, taking some o
University of Texas - BIO - 325
1.23.07 DNA is a polymer, a chain of smaller units, the units are called nucleotides, which have three components Nucleotides: contain a sugar (either deoxyribose or ribose) the defining difference between DNA and RNA (other differences are observed
University of Texas - BIO - 325
1.25.07 So much tension from helicase unwinding that it could cause super coiling, how is the tension resolved? o Topoisomerase is an enzyme that relieves the tension in two ways either Break a phosphodiester bond in one of the two strands to allow
University of Texas - M - 408c
University of Texas - M - 427K
- CHAPTER 2. -Chapter TwoSection 2.1 1a+ba,b Based on the direction field, all solutions seem to converge to a specific increasing function. a- b The integrating factor is .a>b oe /$> , and hence Ca>b oe >$ "* /#> - /$> It follows that all s
University of Texas - EM - em319
304CHAPTER 5Stresses in Beams (Basic Topics)Design of BeamsProblem 5.6-1 The cross section of a narrow-gage railway bridge is shown in part (a) of the figure. The bridge is constructed with longitudinal steel girders that support the wood cros
University of Texas - EM - em319
SECTION 5.7Nonprismatic Beams321Nonprismatic BeamsProblem 5.7-1 A tapered cantilever beam AB of length L has square cross sections and supports a concentrated load P at the free end (see figure on the next page). The width and height of the be
University of Texas - EM - em319
338CHAPTER 5Stresses in Beams (Basic Topics)Shear Stresses in Circular BeamsProblem 5.9-1 A wood pole of solid circular cross section (d diameter) is subjected to a horizontal force P 450 lb (see figure). The length of the pole is L 6 ft, and
University of Texas - EM - em319
350CHAPTER 5Stresses in BeamsBuilt-Up BeamsProblem 5.11-1 A prefabricated wood I-beam serving as a floor joist has the cross section shown in the figure. The allowable load in shear for the glued joints between the web and the flanges is 65 lb
University of Texas - EM - em319
SECTION 5.12Beams with Axial Loads363Problem 5.12-10 A flying buttress transmits a load P 25 kN, acting at an angle of 60 to the horizontal, to the top of a vertical buttress AB (see figure). The vertical buttress has height h 5.0 m and rectang
University of Texas - EM - em319
7Analysis of Stress and StrainPlane StressProblem 7.2-1 An element in plane stress is subjected to stresses 6500 psi, y 1700 psi, and xy 2750 psi, as shown in the x figure. Determine the stresses acting on an element oriented at an angle 60 from
University of Texas - EM - em319
SECTION 7.3Principal Stresses and Maximum Shear Stresses439Problem 7.3-9 A shear wall in a reinforced concrete building is subjected to a vertical uniform load of intensity q and a horizontal force H, as shown in the first part of the figure. (
University of Texas - EM - em319
452CHAPTER 7Analysis of Stress and StrainProblem 7.4-7 An element in pure shear is subjected to stresses 3000 psi, as shown in the figure. xy Using Mohr's circle, determine (a) the stresses acting on an element oriented at a counterclockwise an
University of Texas - EM - em319
466CHAPTER 7Analysis of Stress and StrainProblem 7.5-8 A brass cube 50 mm on each edge is compressed in two perpendicular directions by forces P 175 kN (see figure). Calculate the change V in the volume of the cube and the strain energy U store
University of Texas - EM - em319
9Deflections of BeamsDifferential Equations of the Deflection CurveThe beams described in the problems for Section 9.2 have constant flexural rigidity EI. Problem 9.2-1 The deflection curve for a simple beam AB (see figure) is given by the follow
University of Texas - EM - em319
SECTION 9.4Differential Equations of the Deflection Curve559Differential Equations of the Deflection CurveThe beams described in the problems for Section 9.4 have constant flexural rigidity EI. Also, the origin of coordinates is at the left-ha
University of Texas - EM - em319
SECTION 9.5Method of Superposition571q0Problem 9.5-11 Determine the angle of rotation B and deflection B at the free end of a cantilever beam AB supporting a parabolic load defined by the equation q q0 x 2/L2 (see figure).y ABxLSolut
University of Texas - EM - em319
588CHAPTER 9Deflections of BeamsNonprismatic BeamsProblem 9.7-1 The cantilever beam ACB shown in the figure has moments of inertia I2 and I1 in parts AC and CB, respectively. (a) Using the method of superposition, determine the deflection B at
University of Texas - EM - em319
SECTION 9.9Castigliano's Theorem601Castigliano's TheoremThe beams described in the problems for Section 9.9 have constant flexural rigidity EI. Problem 9.9-1 A simple beam AB of length L is loaded at the left-hand end by a couple of moment M0
University of Texas - EM - em319
SECTION 9.11Representation of Loads on Beams by Discontinuity Functions615Representation of Loads on Beams by Discontinuity FunctionsProblem 9.11-1 through 9.11-12 A beam and its loading are shown in the figure. Using discontinuity functions,
University of Texas - EM - em319
11 #Columns Chapter TitleIdealized Buckling ModelsProblem 11.2-1 through 11.2-4 The figure shows an idealized structure consisting of one or more rigid bars with pinned connections and linearly elastic springs. Rotational stiffness is denoted R a
University of Texas - EM - em319
682CHAPTER 11ColumnsColumns with Other Support ConditionsThe problems for Section 11.4 are to be solved using the assumptions of ideal, slender, prismatic, linearly elastic columns (Euler buckling). Buckling occurs in the plane of the figure u
University of Texas - EM - em319
SECTION 11.9Design Formulas for Columns711Problem 11.9-9 Determine the allowable axial load Pallow for a steel pipe column that is fixed at the base and free at the top (see figure) for each of the following lengths: L 6 ft, 9 ft, 12 ft, and 15
University of Texas - EM - em319
12Review of Centroids and Moments of InertiaDifferential Equations of the Deflection CurveThe problems for Section 12.2 are to be solved by integration.Problem 12.2-1 Determine the distances x and y to the centroid C of a righttriangle having
University of Texas - EM - em319
SECTION 12.6Polar Moments of Inertia15Polar Moments of InertiaProblem 12.6-1 Determine the polar moment of inertia IP of an isosceles triangle of base b and altitude h with respect to its apex (see Case 5, Appendix D) Solution 12.6-1 Polar mom
University of Texas - M - 427K
- CHAPTER 3. -Chapter ThreeSection 3.1 1. Let C oe /<> , so that C w oe < /<> and C ww oe < /<> . Direct substitution into the differential equation yields a<# #< $b/<> oe ! . Canceling the exponential, the characteristic equation is <# #< $ o
University of Texas - M - 427K
- CHAPTER 4. -Chapter FourSection 4.1 1. The differential equation is in standard form. Its coefficients, as well as the function 1a>b oe > , are continuous everywhere. Hence solutions are valid on the entire real line. 3. Writing the equation in
University of Texas - M - 427K
- CHAPTER 5. -Chapter FiveSection 5.1 1. Apply the ratio test : lim aB $b8" k a B $b 8 kHence the series converges absolutely for kB $k " . The radius of convergence is 3 oe " . The series diverges for B oe # and B oe % , since the n-th ter
University of Texas - M - 427K
- CHAPTER 6. -Chapter SixSection 6.1 3.The function 0 a>b is continuous. 4.The function 0 a>b has a jump discontinuity at > oe " . 7. Integration is a linear operation. It follows that (E !-9=2 ,> /=> .> oe" E ,> => " E ,> => ( / / .>
University of Texas - M - 427K
- CHAPTER 7. -Chapter SevenSection 7.1 1. Introduce the variables B" oe ? and B# oe ? w . It follows that B"w oe B# and B#w oe ? ww oe #? !& ? w . In terms of the new variables, we obtain the system of two first order ODEs B"w oe B# B#w oe #B"
University of Texas - M - 427K
- CHAPTER 8. -Chapter EightSection 8.1 2. The Euler formula for this problem is C8" oe C8 2^& >8 $C8 , C8" oe C8 &82# $2 C8 ,in which >8 oe >! 82 Since >! oe ! , we can also writea+b. Euler method with 2 oe !& >8 C8 8oe# !" "&*)! 8oe% !
University of Texas - M - 427K
- CHAPTER 9. -Chapter NineSection 9.1 2a+b Setting x oe 0 /<> results in the algebraic equations OE &< $For a nonzero solution, we must have ./>aA < Ib oe <# ' < ) oe ! . The roots of the characteristic equation are <" oe # and <# oe % . For
Maryland - ENCE - 320
Chapter 10 Recall our discussions on incapacitation-what does it mean? o Depriving an offender of the ability to commit crimes against society, usually by detaining the offender in prison Be able to discern the differences between mandatory sentences
Maryland - ENCE - 320
ENCE 320 Chapter 1 Questions p.19 1. Project: An endeavor to accomplish a specific objective through a unique set of interrelated tasks and the effective utilization of resources 2. Project Objective: An expected result of product 3. Examples of reso
Duquesne - PHIL - IHP 132
Skedzielewski 1 Lisa Skedzielewski Philosophy IHP132-2 Paper Option #1 2007 January 27Socrates introduced Diotema's speech, which he claims taught him mostly everything about he knows about love. Diotema's basic concept centers around the idea that
Harvard - EC - 10
Ec 10 Feldstein LectureSocial Security now: pay as you go Benefit growth: Growth in labor force big problem3/21/2008 12:13:00 PMo Not growing fast enough, slower than baby boomer retiring rate o Possible alternative: raise social security rates
Harvard - EC - 10
Monopolies- closed seller that has no close substitutes *look up how gov controls monopolies 1. How do we have monopolies? a. Gov franchise (Gives some business exclusive rights to deal in that mkt) i. AT&T was the sole phone network for a while. b.
Harvard - EC - 10
Expected Utility Theory12/5/2007 1:22:00 PMErrors of odds Sample size neglect- ignoring the sample from which we're basing our judgements. Gambler's fallacy- believing if you had a string of bad luck that your luck is about to change. Conjunction
Harvard - EC - 10
Least squares regression equation: y=a+bx b=r(Sy/Sx) a=y-bx R^2 x% of variation in Y can be explained by X 5 study elements: object of study, observational or experimental, how individuals are selected, how many individuals, what variables are measu
Harvard - EC - 10
Organizing Scientific Thinking Using the QuALMRI FrameworkWritten by Kevin Ochsner and modified by others. Based on a scheme devised by Steve Kosslyn. This handout outlines a structured process for generating, asking, evaluating and answering scient
Maryland - ENCE - 320
ENCE 320 Chapter 1 WWW Exercises p.20 3. www.pmi.org a. Becoming a member on PMI gives you the benefits of members-only discounts and services, complimentary publications, and continuing education opportunities. Complimentary publications include PM
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Clarkson - ES - 220
Johns Hopkins - PHYS - 171.101
1. The number of atoms per unit volume is given by n = d / M , where d is the mass density of copper and M is the mass of a single copper atom. Since each atom contributes one conduction electron, n is also the number of conduction electrons per unit
Johns Hopkins - PHYS - 171.101
1. With speed v = 11200 m/s, we findK= 1 2 1 mv = (2.9 105 ) (11200) 2 = 18 1013 J. . 2 22. (a) The change in kinetic energy for the meteorite would be1 1 K = K f - K i = - K i = - mi vi2 = - 4 106 kg 15 103 m/s 2 2()()2= -5 1014 J
Johns Hopkins - PHYS - 171.101
1. The speed (assumed constant) is (90 km/h)(1000 m/km) / (3600 s/h) = 25 m/s. Thus, during 0.50 s, the car travels (0.50)(25) 13 m.2. Huber's speed is v0=(200 m)/(6.509 s)=30.72 m/s = 110.6 km/h, where we have used the conversion factor 1 m/s = 3
Johns Hopkins - PHYS - 171.101
1. The air inside pushes outward with a force given by piA, where pi is the pressure inside the room and A is the area of the window. Similarly, the air on the outside pushes inward with a force given by poA, where po is the pressure outside. The mag
Johns Hopkins - PHYS - 171.101
1. The x and the y components of a vector a lying on the xy plane are given byax = a cos , a y = a sin where a =| a | is the magnitude and is the angle between a and the positive x axis. (a) The x component of a is given by ax = 7.3 cos 250 = 2