lecture #2 shear stresses and shear center in multiple closed contour

17
Lecture #2 Shear stresses and shear center in multiple closed contour

Upload: silas-thomas

Post on 18-Dec-2015

239 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: Lecture #2 Shear stresses and shear center in multiple closed contour

Lecture #2Shear stresses and shear centerin multiple closed contour

Page 2: Lecture #2 Shear stresses and shear center in multiple closed contour

SHEAR STRESSES RELATED QUESTIONS

2

- shear flows due to the shear force, with no torsion;

- shear center;

- torsion of closed contour;

- torsion of opened contour, restrained torsion and deplanation;

- shear flows in the closed contour under combined action of bending and torsion;

- twisting angles;

- shear flows in multiple-closed contours.

Page 3: Lecture #2 Shear stresses and shear center in multiple closed contour

SHEAR FLOW IN MULTIPLE-CLOSED CONTOUR.STATIC INDETERMINACY

3

The total shear flow is represented as a sum of variable part qf for an opened contour and shear

flows in separate cells q0i taken with certain sign ̅qi :

Here ̅qi = ±1 and is determined according to positive or

negative tangential coordinate direction.

0f iii

q q q q

If the contour has i closed contours (cells), the problem has i unknown cell flows q0i but it is statically

indeterminate only i-1 times because one unknown could be evaluated from equilibrium equation.

Page 4: Lecture #2 Shear stresses and shear center in multiple closed contour

EQUILIBRIUM EQUATION

4

An equilibrium equation includes i unknown flows in cells q0i :

Here Mq0 , Mqf – moments from constant and variable

parts of shear flow, respectively;MQ – moment from resultant shear force;

i – double area of separate i-th contour.

0i i qf Qi

q M M

0q qf QM M M

Page 5: Lecture #2 Shear stresses and shear center in multiple closed contour

DETERMINATION OF RELATIVE TWIST ANGLES

5

We use the formula derived at last lecture:

1; .t

q qdt q

G

Substituting the sum for shear flow, we get

or

0f j i j

iij jt t

q q q qdt q

G G

0iF ij ii

q

Page 6: Lecture #2 Shear stresses and shear center in multiple closed contour

THE SYSTEM OF EQUATIONS

6

The system of equations includes one equilibrium equation and j = i relative twist angles equations:

0

01

;

, 1, .

i i qf Qi

n

ij i iFi

q M M

q j n

Page 7: Lecture #2 Shear stresses and shear center in multiple closed contour

EXAMPLE – GIVEN DATA

7

EQUIVALENT DISCRETE CROSS SECTION

Page 8: Lecture #2 Shear stresses and shear center in multiple closed contour

8

EXAMPLE – DISCRETE APPROACH

, kN mfq t

1q

2q

= 6.59·10-6 °/N;

= - 9.65·10-7 °/N;

= - 7.07·10-7 °/N;

= 5.84·10-6 °/N;

F= - 0.87 °/m;

2F= - 3.13 °/m.

Page 9: Lecture #2 Shear stresses and shear center in multiple closed contour

EXAMPLE – DISTRIBUTED APPROACH

9

For equilibrium equation, we have:- moment from shear flows qf : Mqf = -47.3 kN·m ;

- moment from resultant shear force Qy :

MQ = -15 kN·m .Solving the system of equations, we get- shear flows in contours q01 = 114.2 kN/m and

q02 = 455.0 kN/m ;

- relative twist angle = - 0.556 °/m (compare to = - 0.473 °/m which we calculated for similar single- closed contour)

Page 10: Lecture #2 Shear stresses and shear center in multiple closed contour

10

, kN mfq t

011 , kN mq q

022 , kN mq q

Page 11: Lecture #2 Shear stresses and shear center in multiple closed contour

11

, kN mq

EXAMPLE – FINAL DIAGRAMFOR DISCRETE APPROACH

Page 12: Lecture #2 Shear stresses and shear center in multiple closed contour

12

, kN mq

EXAMPLE – CONTINUOUS APPROACH , kN mfq t

Page 13: Lecture #2 Shear stresses and shear center in multiple closed contour

13

, kN mq

EXAMPLE – CONTINUOUS AND DISCRETE APPROACHES BEING COMPARED

Page 14: Lecture #2 Shear stresses and shear center in multiple closed contour

14

, kN mq

EXAMPLE – SINGLE-CLOSED AND DOUBLE-CLOSED CONTOURS BEING COMPARED

Page 15: Lecture #2 Shear stresses and shear center in multiple closed contour

SHEAR CENTER CALCULATION

15

Firstly, we solve the following system with arbitrary chosen torsional moment MT :

Next, we find torsion rigidity G·I = MT / T and

0

01

;

, 1, .

i i Ti

n

ij i Ti

q M

q j n

SC Qy

G IX X

Q

Page 16: Lecture #2 Shear stresses and shear center in multiple closed contour

16

EXAMPLE – SHEAR CENTER CALCULATION

shear center

shear center

Page 17: Lecture #2 Shear stresses and shear center in multiple closed contour

TOPIC OF THE NEXT LECTURE

17

Torsion of opened cross sections

All materials of our course are availableat department website k102.khai.edu

1. Go to the page “Библиотека”2. Press “Structural Mechanics (lecturer Vakulenko S.V.)”