Upload
ajaykrishna99
View
215
Download
0
Embed Size (px)
Citation preview
8/14/2019 89589540-Strength-of-Materials-by-S-K-Mondal-14.pdf
1/4
14. Strain Energy Method
Theory at a Glance (for IES, GATE, PSU)1. Resilience (U) Resilience is an ability of a material to absorb energy when
elastically deformed and to return it when unloaded.
The strain energy stored in a specimen when stained within
the elastic limit is known as resilience.
2
U = U =2 2
2
E V o lu m e o r V o lu m e
E
2. Proof Resilience Maximum strain energy stored at elastic limit. i.e. the strain energy stored in the body upto
elastic limit.
This is the property of the material that enables it to resist shock and impact by storing
energy. The measure of proof resilience is the strain energy absorbed per unit volume.
3. Modulus of Resilience (u)The proof resilience per unit volume is known as modulus of resilience. If is the stress due to
gradually applied load, then
2
u = u =2 2
2 E o r
E
4. Application
2 22
22
3P .
4 4= 2 2 (2 ) 2.4 4
L L P
P LU d AE d E E
= +
Strain energy becomes smaller & smaller as the cross sectional area of bar
is increased over more & more of its length i.e. A , U
5. Toughness This is the property which enables a material to be twisted, bent or stretched under impact
load or high stress before rupture. It may be considered to be the ability of the material to
LL/4
2d
P
Page 387 of 429
8/14/2019 89589540-Strength-of-Materials-by-S-K-Mondal-14.pdf
2/4
hapter-14abso
abso
Toug
The
Toug
Thestruc
odulus of
The
to ab
The
that
with
Thediag
whic
be
mate
fract
. Strain
Strain
u
Tota
Cas
Sol
Ho
b energy i
bed after b
hness is an
bility to wi
hness = str
materialstures that
Toughne
ability of u
sorb energy
amount of
the mat
ut failure.
rea under
am is calle
h is a meas
bsorbed b
rial due to i
ures.
nergy in
2
nergy per
or,
2=
G
Strain Ene
12
=
s
s
U
U
or =sU
s
, sid shaft U
,llowshaft
n the plas
ing stresse
ability to a
thstand occ
ngth + duc
ith higheill be expo
s
nit volume
in the plas
work per
erial can
the entire s
modulus o
ure of ener
the unit
mpact load
shear a
2
s
nit volume
u2 = G
rgy (U) for
2
12
T
T Lor
GJ
2max
2
22
LG r
2max
4 =
G
2max
4sU
G=
Strain Eic zone. T
d upto the p
sorb energ
sional stre
ility
modulused to sudde
of material
ic range.
nit volume
withstand
tress strain
f toughness ,
gy that can
volume of
ng before it
d torsio
s, (u )
Shaft in T
21 GJ2
L
2 d
2 L
( 4 42
D d
D
ergy Mete measure
oint of frac
in the plas
ses above t
of toughnen and impa
orsion
) 2max4
L
G=
od of toughn
ure.
tic range.
he yield str
ss are uset loads.
U
( )2 22
D d
D
+
O
T
ss is the
ss without
d to make
= u f
Volume
A
Bd
S K Moamount of
fracture.
componen
ndalsenergy
ts and
Page 388 of 429
8/14/2019 89589540-Strength-of-Materials-by-S-K-Mondal-14.pdf
3/4
Chapter
7. Strai
A
S
o r
C
I
8. Cast
14
s = L
hin walle
here
Conical sp
Cantilever
Helical sp
n energy
ngle subten
rain energ
=
=
0
U2
2
L
b
b
M
E I
ases
o Canti
o Simpl
portant
o For p
o For n
gliones= n
n
U P
,
ngth of me
stube U
S, U
=ring
eam with l
, =sing U
in bendi
ed by arc,
stored in b
2
22
2
.x d xI
d yd x
lever beam
y supporte
ote
re bending
M is cons
MLEI
=
=2
2
M LU
EI
n-uniform
Strain en
Strain en
theorem
Strai2
4an centre li
sLt G
2 2
0
2
P=
2GJ
n
GJ d dx
R
oad 'p' at e
2 3 P R nGJ
ng.
.= x M d EI eam.
d x
with a end l
with a loa
tant along t
if Misknow
bending
ergy in she
ergy in ben
Energy M
e
2
2
( var
= GJ dx
d R
s
3d, U
5
=
( 2= L
2
2
d yd x
oad P , bU
P at centr
he length L
=2
n2
EIif
L
r is neglect
ing is only
ethod
2
0
.
ies with
n PR R
GJ
2
P LbhG
) Rn
=
ME I
2 3
6= P L
EI
,2
96=
b
PU
curvature
ed
considered.
. ( =d R
3
I
/ isknowL
S K
)adius
n
Mondals
Page 389 of 429
8/14/2019 89589540-Strength-of-Materials-by-S-K-Mondal-14.pdf
4/4
Chapter-14 Strain Energy Method S K Mondals1 =
x x
M U M dx
p EI p
Note:
o Strain energy, stored due to direct stress in 3 coordinates
21 ( ) 2 2
= x x y
U E
o = =If ,in case of equal stress in 3 direction thenx y z
2 23 U= [1 2 ] (volume strain energy)
2 2E k =
Page 390 of 429