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An in-depth exploration of torsion and thermal effects in architectural structures. Topics covered include torsional stress and strain, shear stress distribution, shearing strain, torsional stress-strain relationship, and non-circular shapes. The document also discusses open thin-walled sections, shear flow in closed and open sections, deformation relationships, and thermal deformation. It includes coefficients of thermal expansion for various materials and an explanation of stresses and thermal strains when thermal movement is restrained.
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Torsion & Temp 1Lecture 17
A
A
RCHITECTURAL
S
TRUCTURES
I:
S
TATICS AND
S
TRENGTH OF
M
ATERIALS
lecture
Torsion & Temp 2Lecture 17
A
can see torsionalstresses & twistingof axi-symmetricalcross sections^ –
torque
remain plane
undistorted
rotates
-^
not true for squaresections....
T T
related to
is the radial distance from the centroid to the pointunder strain
-^
shear strain varies linearlyalong the radius:
is at
outer diameter
ρφ L
γ =
Torsion & Temp 5Lecture 17
A
know
and
so
-^
where G is the Shear Modulus
ρφ
τ
ρφ^ L
γ =
γ
τ
max
happens at outer diameter
combined shear andaxial stresses^ –
maximum shearstress at 45° “twisted”plane
knowing
and
solve:
-^
composite shafts:
ρφ
τ
ρ
τ =
φ
i i
i i
i^
Σ
φ =
Torsion & Temp 10Lecture 17
A
with very large a/b ratios:
2
13
max
τ
3
13
φ
Torsion & Temp 11Lecture 17
A
q is the internal shear force/unit length
-^
is the area bounded by the centerline
s
i^
is the length segment, t
is the thicknessi
τ
i^
2
φ
Torsion & Temp 13Lecture 17
A
physical movement^ –
axially (same or zero)
rotations from axial changes
-^
relates
to P
steel
20 kN aluminum
aluminum
δ
Torsion & Temp 14Lecture 17
A
atomic chemistry reactsto changes in energy
-^
solid materials
-^
can contract with decrease in temperature
-^
can expand with increase in temperature
linear change canbe measured perdegree
12.8 x 10
Aluminum
10.4 x 10
Brass
10.1 x 10
Bronze
9.3 x 10
Copper
6.7 x 10
Wrought Iron
6.5 x 10
Steel
5.9 x 10
Cast Iron
5.5 x 10
Concrete
4.4 x 10
Glass
3.0 x 10
Wood
Coefficients (
α
) [in./in./
°F]
Material
if thermal movement is restrainedstresses are induced
bar pushes on supports
support pushes back
reaction causes internalstress
E L
P A
f
=
Torsion & Temp 19Lecture 17
A
total length change restrained tozero
T
P
δ
δ (^
)^
Δ
−
L T
PL AE
α
(^
) E T
P A
f^
Δ
α
(^
) L T
T^
Δ
=
α
δ
PL AE
p^
δ
constraint:
sub: