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M

ay

2009

www.read-tpt.com

116

A study into rollforming of

parabolical section

By Dr Jiying Liu, Mr Yuanguang Li and Mr Zhengqing Ai, North China University of Technology, Beijing, China

Supported by Beijing Municipal Natural Science Foundation (3082008)

Abstract

In order to meet precision requirements, the parabola fitting is

achieved by using the smallest arc. Based on the Biswas formula,

the springback model of rollforming parabolic section is a viable

option. It is possible to design the roll flower pattern of parabolic

section. The correctness of the springback model is verified by

experiments and finite element analysis. The rollforming method

can be used for the manufacture of parabolic section in engineering

applications.

Key words:

Parabolic section, rollforming, FEA simulation, Biswas

springback

1. Introduction

Directional light, which is normally present in sectional surface, can

be focused on the focal line by use of a parabolic section. It can

then achieve a highly efficient gathering that puts heat pipe on the

focal line. Based on this feature, parabolic section can be used as a

reflector of solar energy water heater.

The principle drawing is shown in figure 1. Some research shows

that heat energy efficiency of multiple parabolic reflector (composed

of parabolic section), is higher than that of a plane and circle arc

reflector by 60 to 70 per cent

[1] [2]

.

At present, because of

high cost and difficult

forming,

to

some

extent, application of

parabolic

section

is

limited in engineering.

Roll forming is a high

production and low cost

of forming process of

sheet metal. So, using

roll forming technology

to manufacture parabolic

section has positive

signification to industrial

application.

The difficulty of using roll forming technology lies in manufacturing

the section of variable curvature, what with the complexity of

spring back during forming which can not be resolved by existing

technology. Aimed at reflector of solar energy water heater and

combining finite element simulation and experiment analysis,

we have investigated a roll forming method to form parabolic

section.

2. Forming of a parabolic section

In this study, an inside contour of parabolic section is used as the

research object. The mathematical expression of the contour is

The section material is 1060H18 aluminium sheet. The unfolding

width of the section is 120mm, and the thickness is 0.5mm.

Using a circle arc subsection fitting parabolic line, the variable

curvature problem is simplified as a multi-arc problem. When

experiencing a normal error with a maximum limit of less than

0.1mm, the parabolic section can be substituted with 4 arcs. Two

outside arcs are formed first, and then two inside arcs.

Due to this fact, forming with a large radius of thin wall, the

springback must be considered. For fitting a circle arc, the over-

bend forming method should be applied, and the over-bend radius

is calculated by the following formula

[3]

:

(where,

r

f

=

,

r

i

1

= bend radius (mm),

r

i

2

= radius after

springback (mm),

r

f

= yield curvature (mm),

E

= Young’s modulus

(MPa),

t

= thickness of sheet materials (mm),

S

= yield stress of

materials (MPa))

The roll flower pattern is shown in figure 2. It is possible to see that

the third pass is an over-bending forming of the outside arc, and the

ninth pass is over-bending forming in the side arc.

3. Experiments and result analysis

According to the forming of the flower pattern, the rolls were

designed and manufactured, and the experiment carried out by a

rollforming machine at the North China University of Technology

Roll-forming Laboratory (figure 3). The precut length of the

aluminium strip was 1,000mm, width 120mm and thickness 0.48mm.

The formed parabolic section samples are shown in figure 4.

Figure 1

:

Principle drawing of solar energy

reflector with parabolic section

Figure 2

:

Roll flower pattern

1

72

y

=

x

2

,

(–48 ≤

x

≤ 48)

=

1–1.5

+

0.5

3

r

i

1

r

i

2

r

i

1

r

f

r

i

1

r

( )

E

×

t

2

×

S