Torsion and Thermal Effects in Architectural Structures: Lecture 17, Slides of Structural Design and Architecture

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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2011/2012

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Torsion & Temp 1
Lecture 17
A
ARCHITECTURAL STRUCTURES I:
STATICS AND STRENGTH OF MATERIALS
seventeen
torsion
& thermal effects
lecture
docsity.com
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Torsion & Temp 1Lecture 17

A

A

RCHITECTURAL

S

TRUCTURES

I:

S

TATICS AND

S

TRENGTH OF

M

ATERIALS

seventeen torsion& thermal effects

lecture

Torsion & Temp 2Lecture 17

A

Torsional Stress & Strain •^

can see torsionalstresses & twistingof axi-symmetricalcross sections^ –

torque

remain plane

undistorted

rotates

-^

not true for squaresections....

T T

Shearing Strain •^ Torsion & Temp 4Lecture 17

related to

is the radial distance from the centroid to the pointunder strain

-^

shear strain varies linearlyalong the radius:

γmax

is at

outer diameter

ρφ L

γ =

Torsion & Temp 5Lecture 17

A

Torsional Stress - Strain •^

know

and

•^

so

-^

where G is the Shear Modulus

L

G

ρφ

τ

ρφ^ L

γ =

γ

τ

G

f^ v

Shear Stress • Torsion & Temp 7Lecture 17

max

happens at outer diameter

•^

combined shear andaxial stresses^ –

maximum shearstress at 45° “twisted”plane

Shear strain •^ Torsion & Temp 8Lecture 17

knowing

and

•^

solve:

-^

composite shafts:

L

G

ρφ

τ

J

T

ρ

τ =

TL JG

φ

i i

i i

i^

G

J

L

T

Σ

φ =

Torsion & Temp 10Lecture 17

A

Open Thin-Walled Sections •^

with very large a/b ratios:

2

13

max

T ab

τ

G

TL ab

3

13

φ

Torsion & Temp 11Lecture 17

A

Shear Flow in Closed Sections •^

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

a t

T

τ

i^

i ti

s

TL t

2

a

φ

a

Torsion & Temp 13Lecture 17

A

Deformation Relationships •^

physical movement^ –

axially (same or zero)

rotations from axial changes

-^

relates

to P

steel

20 kN aluminum

aluminum

PL AE

δ

Torsion & Temp 14Lecture 17

A

Deformations from Temperature •^

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

Coefficients of Thermal ExpansionTorsion & Temp 16Lecture 17

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

Stresses and Thermal Strains •^ Torsion & Temp 17Lecture 17

if thermal movement is restrainedstresses are induced

bar pushes on supports

support pushes back

reaction causes internalstress

E L

P A

f

δ

=

Torsion & Temp 19Lecture 17

A

Superposition Method –^

total length change restrained tozero

0

T

P

δ

δ (^

)^

0

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: