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S.1Strength of Materials (April/May-2013, Set-1) JNTU-Kakinada
( JNTU-Kakinada ) B.Tech. II-Year II-Sem.
Code No.: R22012/R10
II B.Tech. II Semester Regular Examinations
April/May - 2013
STRENGTH OF MATERIALS
( Civil Engineering )
Time: 3 Hours Max. Marks: 75
Answer any FIVE Questions
All Questions carry Equal Marks
- - -
1. (a) Using the moment-area method, determine the deflection at the free end of a cantilever beam of span l subjectedto a load P at a distance a from the fixed end. El is constant. (Unit-I, Topic No. 1.5)
(b) Derive the differential equation of the elastic curve for a beam subjected to bending in a plane of symmetry.[5+10] (Unit-I, Topic No. 1.1)
2. (a) Derive expression for volumetric change in thin cylinder subjected to an internal pressure p.(Unit-II, Topic No. 2.1.1)
(b) A thick cylindrical pipe of outside diameter 300 mm and internal diameter 200 mm is subjected to an internal fluidpressure of 14 MPa. Determine the maximum hoop stress in the section. Draw the variation of the hoop stressacross the thickness of the pipe. [7+8] (Unit-II, Topic No. 2.2)
3. A square element of a thin plate subjected to a compressive stress of 5 MPa in x-direction, a tensile stress of 15 MPain y-direction and a shear stress of 10 MPa (clockwise). Determine the principal stresses and their directions by usinganalytical method. Also find the normal stress and shear stress on the diagonal plane of the square element. [15](Unit-III, Topic No. 3.2)
4. A closed coil helical spring is made of 12 mm diameter wire and is having mean diameter of 150 mm and 10 completeturns. The modulus of rigidity of the material of spring is 80 MPa. When a load of 500 N is applied, determine themaximum shear stress, strain energy stored, deflection produced and stiffness of the spring. [15](Unit-IV, Topic No. 4.2.2)
5. A built-up I section has the following dimensions,
Overall depth : 400 mm
Flanges : 300 mm × 50 mm
Web thickness : 30 mm
When it is used as a simply supported beam, it deflects by 10 mm when subjected to a load of 40 kN/m over its entirelength? Find the safe load, if the same section is used as a column with both ends hinged. Use Euler’s formula.Assume a factor of safety 1.75 and take E = 2 × 105 MPa. [15] (Unit-V, Topic No. 5.1.2)
6. The cross-section of a masonry pier is a hollow rectangle, the dimensions of external and internal rectangles being1200 mm × 800 mm and 900 mm × 500 mm respectively. A load of 300 kN in the vertical plane bisecting the 1200 mmwidth of pier is transmitted at an eccentricity of ‘e’. Calculate the maximum value of ‘e’ so that no tension is inducedin the section. [15] (Unit-VI, Topic No. 6.2)
Set-1Solutions
S.2 Spectrum ALL-IN-ONE Journal for Engineering Students, 2014
B.Tech. II-Year II-Sem. ( JNTU-Kakinada )
7. Determine the maximum positive bending moment and maximum twisting moment in a semi-circular beam simplysupported on three equally spaced supports. Take radius of the centre line of the beam as ‘R’ and load per unit lengthof the beam as ‘w’. [15] (Unit-VII, Topic No. 7.2.2)
8. Determine the forces in all the members of the truss as shown in the figure. [15] (Unit-VIII, Topic No. 8.2)
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
Figure
S.3Strength of Materials (April/May-2013, Set-1) JNTU-Kakinada
( JNTU-Kakinada ) B.Tech. II-Year II-Sem.
SOLUTIONS TO APRIL/MAY-2013, SET-1, QPQ1. (a) Using the moment-area method,
determine the deflection at the free endof a cantilever beam of span l subjectedto a load P at a distance a from thefixed end. El is constant.
Answer : April/May-13, Set-1, Q1(a) M[5]
Note : In the given reference replace W with P.
For answer refer Unit-I, Q24.
(b) Derive the differential equation of theelastic curve for a beam subjected tobending in a plane of symmetry.
Answer : April/May-13, Set-1, Q1(b) M[10]
For answer refer Unit-I, Q1.
Q2. (a) Derive expression for volumetricchange in thin cylinder subjected to aninternal pressure p.
Answer : April/May-13, Set-1, Q2(a) M[7]
For answer refer Unit-II, Q3.
(b) A thick cylindrical pipe of outsidediameter 300 mm and internal diameter200 mm is subjected to an internal fluidpressure of 14 MPa. Determine themaximum hoop stress in the section.Draw the variation of the hoop stressacross the thickness of the pipe.
Answer : April/May-13, Set-1, Q2(b) M[8]
Given that,
Outer diameter = 300 mm
Inner diameter = 200 mm
Internal pressure = 14 MPa
Required
(i) Maximum hoop stress in a section
(ii) Representation of variation of hoop stressacross thickness of the pipe.
150 mm
100 mm
150 mm
100 mm
Thickness
Let,
Px= Radial pressure
fx
= Hoop stress.
Px=
2x
B – A and f
x = 2x
B + A
At, x = 100 mm , P100
= 14 MPa
x = 0 mm , P0
= 0
x = 150 mm , P150
= 0
Radial stress Px at x = 100 is,
P100
= 2)100(
B – A
14 = 2)100(
B – A ... (1)
Px at x = 150 is,
P150
= 2)150(
B – A
0 = 2)150(
B – A ... (2)
On solving equations (1) and (2) we get,
A = 11.2
B = 252000
Hoop stress,
fx
= 2x
B + A
f100
= 2)100(
252000 + 11.2
= 36.4 N/mm2
f150
= 2)150(
252000 + 11.2
= 22.4 N/mm2
S.4 Spectrum ALL-IN-ONE Journal for Engineering Students, 2014
B.Tech. II-Year II-Sem. ( JNTU-Kakinada )
The maximum hoop stress is developed at the innersurface.
f110
= 2)110(
252000 + 11.2 = 32.026 N/mm2
f120
= 2)120(
252000 + 11.2 = 28.7 N/mm2
f130
= 2)130(
252000 + 11.2 = 26.11 N/mm2
f140
= 2)140(
252000 + 11.2 = 24.054 N/mm2
36.4
36.422.424.126.11
28.732
22.4
140
130
120110150 100
Thickness 100 mm
150 mm
fx
36.4
36.422.424.126.11
28.732
22.4
140
130
120110150 100
Thickness 100 mm
150 mm
fx
Figure: Representation of Hoop Stress Across the Thickness of
Pipe
Q3. A square element of a thin plate subjectedto a compressive stress of 5 MPa in x-direction, a tensile stress of 15 MPa in y-direction and a shear stress of 10 MPa(clockwise). Determine the principal stressesand their directions by using analyticalmethod. Also find the normal stress andshear stress on the diagonal plane of thesquare element.
Answer : April/May-13, Set-1, Q3 M[15]
Given that,
Stress acting on x-axis, σx = – 5 N/mm2
Stress acting on y-axis, σy = 15 N/mm2
Shear stress τxy
= 10 N/mm2 (Clockwise)
Required,
(i) Principal stress and their directions
(ii) Normal stress and shear stress on the diagonalplane of the square elements.
(i) Principal Stress and their Direction
Principal stress,
(σ1, σ
2) =
2yx σ+σ
± 2
2
2
–xy
yx τ+
σσ
σmax
= σ1
= 2
yx σ+σ +
22
2
–xy
yx τ+
σσ
= 2
15)5(– + +
22
)10(2
15–)5(– +
= 5 + 100100 += 19.14 N/mm2
σmin
= σ2
=
σ+σ2
yx –
22
2
–xy
yx τ+
σσ
= 2
155– + –
22
)10(2
15–5– +
= 5 – 100100×
σ2
= – 9.14 N/mm2
The angle made by principal plane and shear stresswith x-axis is,
tan2θ = yx
xy
σστ–
2–
= 15–5–
102– ×
tan2θ = 1
θ = 2
)1(tan 1–
θ = 22°30'00'
θ1= 90 + θ
θ1= 112°30'00'
S.5Strength of Materials (April/May-2013, Set-1) JNTU-Kakinada
( JNTU-Kakinada ) B.Tech. II-Year II-Sem.
(ii) Normal Stress and Shear Stress on the DiagonalPlane of the Square Element
Normal stress on the diagonal of the square element(σ
n) (i.e., θ = 45°) is,
σn
=
σ+σ2
yx +
σσ2
– yxcos2θ + τ
xy sin2θ
=
+
2
15)5(–+
2
15–)5(–cos(2 × 45) + 10 sin(2 × 45)
= 5 + (– 10) cos90 + 10 sin90
= 15 N/mm2
Shear stress on the diagonal of square element is,
τxy
=
σσ2
– yxsin2θ + τ
xy cos2θ
=
2
15–)5(–sin(2 × 45) + 10 cos(2 × 45)
= – 10 sin90 + 10 cos90
= – 10 N/mm2
Q4. A closed coil helical spring is made of 12mm diameter wire and is having meandiameter of 150 mm and 10 complete turns.The modulus of rigidity of the material ofspring is 80 MPa. When a load of 500 N isapplied, determine the maximum shearstress, strain energy stored, deflectionproduced and stiffness of the spring.
Answer : April/May-13, Set-1, Q4 M[15]
Given that,
Diameter of steel wire, d = 12 mm
Number of turns in spring, n = 10
Mean diameter, D = 150 mm
Mean radius, R = 75 mm
Modulus of rigidity, G = 80 N/mm2
Load, W = 500 N
Required,
(i) Maximum shear stress
(ii) Deflection produced
(iii) Strain energy stored
(iv) Stiffness of the spring.
(i) Maximum Shear StressThe maximum shear stress (τ) is given by equation,
WR = 16
π × τ × d3
500 × 75 = 16
π × τ × (12)3
τ = 110.52 N/mm2
(ii) Deflection ProducedDeflection in the spring,
δ = 4
364
Gd
nWR
δ = 4
3
1280
107550064
××××
= 81380.20 mm
∴ δ = 81.3 m
(iii) Strain Energy StoredStrain energy stored,
u = 2
1Wδ
= 2
1 × 500 × 81.3
∴ u = 20325 N-m
(iv) Stiffness of the Spring Stiffness of the spring,
S = δ
W
= m3.81
500
= 6.15 N/m
Q5. A built-up I section has the followingdimensions.
Overall depth : 400 mmFlanges : 300 mm × 50 mmWeb thickness : 30 mm
When it is used as a simply supported beam,it deflects by 10 mm when subjected to aload of 40 kN/m over its entire length. Findthe safe load, if the same section is used asa column with both end hinged. Use Euler’sformula. Assume a factor of safety as 1.75and take E = 2 × 105 MPa.
S.6 Spectrum ALL-IN-ONE Journal for Engineering Students, 2014
B.Tech. II-Year II-Sem. ( JNTU-Kakinada )
Answer : April/May-13, Set-1, Q5 M[15]
300 mm
300 mm
400 mm 30mm
300 mm
50 mm
50 mm
135 mm
300 mm
300 mm
400 mm 30mm
300 mm
50 mm
50 mm
135 mm
Given that,
Load, W = 40 kN/m
Deflection, δ = 10 mm
Factor of safety = 1.75
E = 2 × 105 N/mm2
Required
Safe load for the beam
Assume, length of the beam = L
Moment of inertia I-section about x-axis is,
Ix=
×12
400300 3
– 2 ×
×12
300135 3
= 16 × 108 – 60.75 × 107
= 99.25 × 107 mm4
Moment of inertia of the section about y-axis is,
Iy= 2
Flange
3
12
db +
Web
3
12
db
Iy= 2
×12
30050 3
+
×12
30300 3
= 22.5 × 107 + 67 500
= 22.5067500
= 22.5 × 107
Deflection, δ = EI
WL
384
5 4
I : Greatest between Ix and I
y of the section.
(Here I = Ix)
10 = 75
46
1025.99102384
10405
××××××× L
l = 248.47 mm
∴ Length of the beam = 248.47 mm
Finding the safe load when beam is used as a columnwith both the ends hinged. When both the ends are hinged,using Eulers formula,
PEulers
= 2
2
l
EI yπ
= 2
752
)47.248(
105.22102 ××××π × 10– 6 kN
∴ Load, P = 7193.8 kN
–~ 7194 kN
Safe load = safety ofFactor
EulerP
= 75.1
7194
= 4110.80 kN
Q6. The cross-section of a masonry pier is ahollow rectangle, the dimensions of externaland internal rectangles being 1200 mm × 800mm and 900 mm × 500 mm respectively. Aload of 300 kN in the vertical plane bisectingthe 1200 mm width of pier is transmitted atan eccentricity of ‘e’. Calculate the maximumvalue of ‘e’ so that no tension is induced inthe section.
Answer : April/May-13, Set-1, Q6 M[15]
Given that,
In a masonry pier of hollow rectangular section
Dimensions of external rectangle,
B × D = 1200 × 800 mm
Dimensions of internal rectangle,
b × d = 900 mm × 500 mm
S.7Strength of Materials (April/May-2013, Set-1) JNTU-Kakinada
( JNTU-Kakinada ) B.Tech. II-Year II-Sem.
In case of hollow rectangular section,
Area = BD – db
= (1200 × 800) – (900 × 500)
A = 51 × 104 mm2
1200 mm
800 mm500 mm
e
900 mm
1200 mm
800 mm500 mm
e
900 mm
Moment of inertia at XX,
IXX
= 12
3BD –
12
3bd
= 12
8001200 3× –
12
500900 3×
= 4.1825 × 1010 mm4
IXX
= 41825 × 106 mm4
IYY
= 12
3DB –
12
3db
= 12
1200800 3× –
12
900500 3×
IYY
= 8.4825 × 1010 mm4
= 84825 × 106 mm4
ZXX
= maxy
I XX
= D
bdBD
6
– 33
= 8006
500900–8001200 33
×××
ZXX
= 10456.25 × 104 mm4
ZYY
= maxy
IYY
= B
dbDB
6
– 33
= 12006
900500–1200800 33
×××
ZYY
= 14137.5 × 104 mm4
Condition for no tension,
e ≤ b
KYY22
Radius of gyration,
2YYK =
A
IYY
= 4
6
1051
1084825
××
2YYK = 1663.25 × 102 mm
Eccentricity, e ≤ b
KYY22×
≤ 900
1025.16632 2××
≤ 369.61 –~ 370
e ≤ 370 mm
Result
Maximum value of eccentricity,
e = 370 mm.
Q7. Determine the maximum positive bendingmoment and maximum twisting moment ina semi-circular beam simply supported onthree equally spaced supports. Take radiusof the centre line of the beam as ‘R’ and loadper unit length of the beam as ‘w’.
Answer : April/May-13, Set-1, Q7 M[15]
For answer refer Unit-VII, Q25.
S.8 Spectrum ALL-IN-ONE Journal for Engineering Students, 2014
B.Tech. II-Year II-Sem. ( JNTU-Kakinada )
Q8. Determine the forces in all the members ofthe truss as shown in the figure.
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
Figure
Answer : April/May-13, Set-1, Q8 M[15]
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
30 kN20 kN 20 kN
40 kN
J I H G F
E
4 m
AB C D
16 mm 4 @ 4 m
Calculation of forces in the members of the truss are,
Reactions
RA + R
E= 30 + 20 + 20 + 40
= 110 kN ... (1)
Taking moments about ‘A’,
ΣME
= 0
RA × 16= 40 × 12 + 20 × 8 + 20 × 4
RA × 16= 480 + 160 + 80
RA × 16= 720
RA
= 16
720
RA= 45 kN
Substitute RA in equation (1), we get,
RA + R
E= 110 kN
45 kN + RE
= 110
RE
= 110 – 45
RE
= 65 kN
By using method, of joints.
At Joint ‘A’
Free body diagram of joint ‘A’,
45°
30 kN
20 kN
A B
J I
45°
30 kN
20 kN
A B
J I
Taking forces vertically,
ΣFy
= 0
FAJ
= 30 kN ; FAI
= 20 kN
Taking forces horizontally,
ΣFx
= 0
FAB
× cos45°= RA × 4
FAB
= °×45cos
445
FAB
= 254.55 kN
At Joint ‘B’
Free body diagram of joint ‘B’,
C
HI
BA C
HI
BA
Taking forces horizontally.
ΣFx
= 0
FAB
+ FBC
× cos45° = 0
254.55 + FBC
cos45° = 0
FBC
= °45cos
55.254–
FBC
= – 360 kN (Compression).
S.9Strength of Materials (April/May-2013, Set-1) JNTU-Kakinada
( JNTU-Kakinada ) B.Tech. II-Year II-Sem.
Taking forces vertically,
ΣFy
= 0
FBI
– FBH
sin45° = 0
FBH
= °45sin
20
= 28.284 kN
FBI
= 20 kN
FBH
= 28.284 kN
At Joint ‘C’
Free body diagram of joint ‘C’,
D
H
CB
20 kN
D
H
CB
20 kN
FCH
= – 20 kN (Compression)
Taking forces horizontally,
FBC
+ FCD
× cos45° = 0
– 360 + FCD × cos45° = 0
FCD
= °45cos
360
FCD
= 509.11 kN
At Joint ‘D’
Free body diagram of joint ‘D’,
E
HG
DC E
HG
DC
Taking forces horizontally,
ΣFx= 0
FCD
+ FDE
– RE × 4 = 0
509.11 + FDE
= 65 × 4
FDE
= – 249.11 kN
Taking forces vertically,
ΣFy
= 0
FGD
= 40 × 4
= 160 kN
– FHD
× sin45° – FGD
= 0
– FHD
= °45sin
160
= 226.27 kN
FHD
= – 226.27 kN
At Joint ‘E’
Free body diagram of joint ‘E’,
GF
ED
45°
65 kN
GF
ED
45°
65 kN
FDE
× 4 – 20 × 4 + RE × 4 + F
FE = 0
– 249.11 × 4 – 80 + 65 × 4 + FFE
= 0
– 816.44 + FFE
= 0
FFE
= 816.44 kN (Tension)
At Joint ‘F’
Free body diagram of joint ‘F’,
G F
E
G F
E
S.10 Spectrum ALL-IN-ONE Journal for Engineering Students, 2014
B.Tech. II-Year II-Sem. ( JNTU-Kakinada )
Taking moments,
– FFE
+ FGF
× 4 = 0
– 816.44 + 4FGF
= 0
FGF
= 4
44.816
FGF
= 204.11 kN (Tension)
At Joint ‘G’
Free body diagram of joint ‘G’,
GH F
D
FGD
GH F
D
FGD
Moment at ‘G’,
FGD
= 40 × 4
= 160 kN
Taking forces horizontally,
FGF
+ FHG
× 4 = 0
204.11 + 4FHG
= 0
FHG
= 4
11.204–
FHG
= – 51.027 kN
At Joint H
Free body diagram of joint H,
HI G
C DB
HI G
C DB
Taking forces horizontally,
FBI
= 20 kN
FIH
+ FHG
× cos45° = 0
FIH
= – 51.027 × cos45°
FIH
= – 36.081 kN (Compression)
At Joint I
Free body diagram at joint I,
IJ H
BA
IJ H
BA
Taking forces horizontally,
ΣFx
= 0
FJI + F
IH cos45° = 0
FJI
= – 36.081 × cos45°
FJI
= – 25.513 kN (Compression)