MECHANICS OF SOLIDS-SOLVED NUMERICALS
Numericals on - Axial load and mechanical properties of materials
Q-1 Determine the dilatation (bulk modulus) e and the change in volume of the 200 mm length of the rod shown if (a) the rod is made of steel with E = 200 GPa and v = 0.30, (b) the rod is made of aluminum with E = 70 GPa and v = 0.35.
Sol 1:
a).
ANS:
WE HAVE :
E = 200 GPa = 2 x 10^5
L = 200 mm
u = 1/m = 0.3
Stress, σ
=P/A = 46 x 10^3 x 4 / 3.14 x (22)^2
= 121.01 N/m
Also, strain (e) = stress (σ) / E
=
121.01 / 2 x10^5
e = 6.05 x 10^-4
= 2 x10^5 / 3(1 – 0.6)
= 2 x 10^5 / 1.2 = 1.6 x 10^5
Then, Strain of dia. = 0.121 / 200 = 0.000605
d d = 0.000605 x 22
= 0.01331.
Then , dv = ( d^2 x dl + 2 l d d d) π/4
= {( 22)2 x 0.121 + 2 x 200 x 22 x 0.01331) π/4}
= 551.95 / 4 = 137. 988
E = 70 GPa = 70 x
109 x10-6 N/m
= 70 x 103 N/m
L = 200 mm
u = 1/m = 0.35
Stress, σ =P/A = 46 x 103 x
4 / 3.14 x (22)2
=
121.01 N/m
Also, strain (e) = stress (σ) / E
= 121.01 / 70 x10^3
e = 1.72 x 10^-3
also, bulk modulus = K= E / 3(1-2/m)
= E/ 3(1 – 0.7)
= E/
0.9
= 7 x
104
=
77777.77 = 7.77 x 10^4 N/m
d d = 1.72 x 10^-3 x 22
= 0.03784.
= 1046.1
/ 4 = 261.525
Q-2 A standard tension test is used to determine the properties of an
experimental plastic. The test specimen is a 15-mm-diameter rod and it is
subjected to a 3.5 kN tensile force. Knowing that an elongation of 11 mm and a
decrease in diameter of 0.62 mm are observed in a 120-mm gage length, determine
the modulus of elasticity, the modulus of rigidity, and Poisson’s ratio of the
material.
Sol2:
D=15mm
P=3.5KN=3.5
x 10^3N
δl =11mm
Change
in diametr=0.62 mm
Gauge length=120 mm
To find : E=?
C=?
POISSON’S
RATIO=?
We know that,
σ =P/A
σ =3.5X10^3 x 4/3.14 x 225
σ =19.81 N/m
Longitudinal strain = e =δl/l
e =11/120
e
=.091
E=σ/e
E=19.81/.091
E=217.62 N/m
Lateral
strain= change in lateral dimension / original lateral dimension
=
0.62/15
= 0.041
Poisson’s
ratio =1/m=lateral strain/longitudional strain
=.041/.091
=0.45
Let C be the modulus of
rigidity
E=2C(1+1/m)
217.32=2C(1+0.45)
Then
, C = 108.66/ 1.45 = 74.93 N/m
Q-3 Using E = 200 GPa, determine (a) the strain energy of the steel rod ABC when P = 25 kN, (b) the corresponding strain-energy density of portions AB and BC of the rod.
Sol 3:
Aab = 3.14/4 x (20)^2
= 314.16 m
Abc = .14/4 x (16)^2
= 201.06 m
Also, p = 25 x 10^3 N.
U = E P^2L/2EA , here E = sigma
= (25 x
10^3)^2 x 1.2 /
2 x (200 x 10^9 ) x 3.14 x10^-6
.+ (25 x 10^3)^2 x 0.8 / 2 x (200 x 10^9) x 201.06 x10^-6
a). U = 5.968 + 6.213 = 12.18 Nm = 12.18 J.
b). STRESSab = 25 x 10^3 / 3.14 x10^-6 = 79.58 x 10^6 Pa.
Uab = (STRESSab)^2
/2E = (79.58 x 10^6)^2 / 2 x 200 x 10^9.
= 15.83 x 10^3 = 15.83 kJ/㎥.
c). STRESSbc = 25 x 10^3 / 201.06 x 10^-6 = 124.28x 10^6 Pa.
Ubc = (STRESSbc)^2
/2E = (124.28 x 10^6)^2 / 2 x 200 x 10^9.
= 38.6 x 10^3 = 38.6
kJ/㎥.
Q-4 Two bars of length L and of same material are subjected to the axial tensile force P. The first bar has a uniform diameter of 2d. The second bar has a diameter d for a length L/3 and a diameter 2d for the remaining length. Compare strain energies of two bars?
Sol 4: For first bar:
Diameter = 2d
Stress = p /3.14
x (2d)^2.
= p/ 3.14 x (d)^2
Here, π = 3.14
Now, Strain energy stored = (stress)^2/
2E x volume of bar.
= 1/ 2E x (p)^2/ (3.14)^2 x (d)^4 x
3.14(2d)^2 l/4
= (p)^2 l/ 2E x 3.14(d)^2.
For second bar:
Then, stress in the part AB = p/ 3.14/4 x (d)^2
= 4p/ 3.14 x d^2.
Also,
stress in the part BC = p/ 3.14/4 x (2d)^2
= p/ 3.14 x d^2.
Now, strain energy stored = strain energy stored by AB + strain energy stored BC.
=
(stress1)^2/ 2E x volume of AB + (stress2)^2/
2E x volume of BC.
= 16p^2/(3.14)^2 (d)^4
x l/2E x 3.14 d^2/4 x l/3
+ p^2/(3.14)^2 (d)^4 x l/2E x 3.14 (2d)^2/4 x2 l/3
= 2/3 x(3.14)^2 l /2E x 3.14 d^2 + 1/3 x(3.14)^2 l /2E x 3.14 d^2
= (3.14)2 l / E x 3.14 d^2.
Therefore, Ratio of strain energies of two bars = p^2 l / 2E 3.14 d^2 x E
3.14 / p^2 l
= 1/2
Q-5 A steel specimen 1.5 c㎡ in cross-
section, stretches 0.005 cm over a 5 cm gauge length under an axial load of 30
KN. Calculate strain energy stored in the specimen at this point. If the load
at the elastic limit for the specimen is 50 KN, calculate the elongation at
elastic limit and proof resilience.
Sol5 :
A = 1.5
c㎡ = 150 m㎡.
dl = 0.005 cm = 0.05 mm.
l =
5 cm = 50 mm
p =
30 kN= 30 x 1000 = 30000 N
Load at elastic limit = 50 KN = 50000 N
Now, Strain energy stored = work done = 1/2 p (dl)
= 1/2 x 30000 x 0.005 = 750 Nmm
= 0.75Nm
We have , elongation due to 30 kN = 0.05 mm
Then , elongation due to 50 kN = 50/30 (0.005) = 10/ 6
(0.005)
= 5/
3 (0.005)
= 1/12 mm = elongation at elastic limit.
Proof
resilence = work done = 1/2 x (load at
elastic limit) x ( extension )
=
1/2 x 50000 x 1/12
= 2083.3 Nmm.
= 2.083 Nm
=
2.083 J
Sol6:
GIVEN:
L=3m=3 x 10^3mm
D=60mm
Es=2
x 10^5N/mm2
To find:
GRADUALLY
STRESS?
ELONGATION?
We know that:
Gradually stress =σ= P/A
σ
=200x10^3x4/3.14x60x60
σ =70.77
e
=σ/E
e =70.77/2 x 10^5
e = 35.88 x 10^-5
δl =e x l
δl =35.88 x 10^-5x 3 x 10^3
δl =1.06 mm
Also. suddenly load is double to gradually load
σ =141.54 N/m
δl =2.12 mm2
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