bredt-batho theory a

35
AE3011 Semester 1; 2012/13 By Jan Niklewicz CEng. MIMechE [email protected] Aerospace Structures and Mechanics

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AE3011

Semester 1; 2012/13

By

Jan Niklewicz CEng. MIMechE

[email protected]

Aerospace Structures and Mechanics

Jan Niklewicz

Managing Director JNDC Ltd Specialist Engineering and Product design Company

Mainly in the Aerospace field

Managing Director Kwikbolt Ltd Design and development and supply of specialist slave fasteners for the

aerospace industry Clients: Lockheed Martin, Airbus, Rolls-Royce, Leyland Trucks, MEP, Rediweld Ltd as

well us individuals and SME’s

Previous Director of Mechanical Engineering at KU

Lead Engineer –Composites centre NP

MSc Imperial College

BEng(Hons) Kingston University

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

volumeG

U S 2

2

When a material is subjected to a shear

stress, τ, the strain energy stored is given

by :

Hence, the energy stored in an axial

element of length L, width ds and thickness

t (see Figure 1) is :

dstLG

U S2

2

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

The total strain energy, U, in the tube will be

given by:

i.e.

where q= t is the shear flow which will be

constant around the section .

t

ds

G

tL = ds t L

G= U 22

222

t

ds

G 2

Lq = U

2

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

The force on the element ds is

τtds = qds .

Taking moments about O gives:

qpds = 2qdA since

Integrating gives :

T = 2Aq

Therefore

ds p 2

1 = dA

dA q 2 = T

2A

T = q

tA

T = 2

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

If the tube twists through an angle, θ, the

work done will be given by :

Equating the work done to the total

internal strain energy gives:

ie:

T 2

1 = WD

t

ds

G 2

Lq = T

2

12

t

ds

GA

TL =

t

ds

GT

Lq =

2

24

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

This equation can be written in the form:

where J is the torsional constant of the

tube given by

JG

L T =

t

ds

AJ

24

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

Hence the rate of twist per unit length

will be given by :

t

ds

2AG

q =

dz

d =

L

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory) Example 1

A 5 m long tailplane has the uniform cross-section shown in Figure Q1. It is

subjected to a torque of 50 kNm. Find the shear stress distribution around

the section and the angle of twist throughout the length assuming that the

centre of twist lies at the centroid of the section. Take G = 30 GPa.

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

Torsion of Closed, Thin-walled Tubes

(Bredt-Batho Theory)

Torsion of Multi-cell Tubes

t

ds

AG

q

dz

d

2

For single cell tubes : T = 2Aq

And

These equations may be adapted for multi-cell tubes

as follows :

Torsion of Multi-cell Tubes

The applied torque T will be the sum of the torques induced in the individual cells i.e.

R

N

R

RqAT

1

2

Torsion of Multi-cell Tubes

and the angle of twist can be determined from

G Constant

G Variable

AR = enclosed area of cell R

qR = shear flow in the Rth cell

δR-1 , R = for the walls common to the (R – 1)th and Rth cells .

RRRRRRRR

R

qqqGAdz

d,11,11

2

1

RR

RR

R

R

RR

RR

RR

R

R Gq

Gq

Gq

Adz

d

,1

,1

1

,1

,1

12

1

t

ds

Torsion of Multi-cell Tubes

Note that at any junction, for equilibrium q1 = q2 + q3.

Torsion of Multi-cell Tubes

Example 2

The tailplane in Example 1 is modified to form a 2-cell section as shown in Figure Q2.

Find the shear stress distribution and the angle of twist over a 5 m length of the

section. Take G = 30 GPa.

Torsion of Multi-cell Tubes

Let shear flows in cells and be q1 and q2 respectively.

A1 = ½(150 + 300) × 200 = 45000 mm2

A2 = ½(300 + 150) × 300 = 67500 mm2

Cell :

RRRRRRRR

R

qqqGAdz

d,11,11

2

1

Cell:

RRRRRRRR

R

qqqGAdz

d,11,11

2

1

1 2

2

1389.2 50

2 67500

dq q

dz G

Compatibility: 1 2

d d

dz dz

Example 3

Calculate the shear stress distribution

in the walls of the three-cell tube

shown in the diagram when it is

subjected to an anticlockwise

torque of 12 kNm. Assume Bredt-

Batho theory holds and that the

tube has the properties shown in

the table below.

1, 1,

1 1

1, 1,

1

2

R R R RRR R R

R R R R R R

dq q q

dz A G G G

1, 1,

1 1

1, 1,

1

2

R R R RRR R R

R R R R R R

dq q q

dz A G G G

1, 1,

1 1

1, 1,

1

2

R R R RRR R R

R R R R R R

dq q q

dz A G G G

Tutorial Examples

Tutorial Examples