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JOURNAL OF COMPUTERS, VOL. 8, NO. 6, JUNE 2013 1507<br />

model. Consider<strong>in</strong>g the symmetry of the mechanism, the<br />

mathematical model is simplified as shown <strong>in</strong> Fig. 4(a).<br />

The support<strong>in</strong>g leg could be simplified to the two-force<br />

bar [12-14]. The force on the p<strong>in</strong> A that is contacted with<br />

the pipe wall is analyzed <strong>in</strong> Fig. 4(b). Accord<strong>in</strong>g to the<br />

pr<strong>in</strong>ciple of force balance, the force can be expressed as<br />

∑ F ( 0) = F x + Fy<br />

= 0<br />

(1)<br />

( ) − F × ( θ + θ ) L<br />

F x = F2 × L × s<strong>in</strong> θ 1 1 s<strong>in</strong> 1 2 × (2)<br />

( )<br />

F y = f × F2 × cos θ 2<br />

(3)<br />

F = F s<strong>in</strong>( )<br />

(4)<br />

1 0 2 θ2<br />

Where F is the resultant force; F 0 is the force produced<br />

by the spr<strong>in</strong>g on the lower support<strong>in</strong>g plate; F 1 is the<br />

support<strong>in</strong>g force of the support<strong>in</strong>g leg; F 2 is the force on<br />

the support<strong>in</strong>g mechanism by the pipe wall, L is the<br />

length of the upper support<strong>in</strong>g leg, f is the friction<br />

coefficient between pipe wall and support<strong>in</strong>g mechanism;<br />

θ 1 is the angle of the upper support<strong>in</strong>g leg to the<br />

horizontal l<strong>in</strong>e; θ 2 is the angle of the lower support<strong>in</strong>g leg<br />

to the horizontal l<strong>in</strong>e.<br />

The force on the support<strong>in</strong>g mechanism by the pipe<br />

wall F 2 can be achieved by Equation (1), (2), (3) and (4)<br />

and expressed as<br />

F0<br />

s<strong>in</strong>( θ1<br />

+ θ2)<br />

F2<br />

= (5)<br />

2(s<strong>in</strong>θ<br />

− f cosθ<br />

)<br />

From Equation (5), the force on the support<strong>in</strong>g<br />

mechanism by the pipe wall F 2 is related to the force<br />

produced by the spr<strong>in</strong>g on the lower support<strong>in</strong>g plate F 0<br />

and the angle of the upper support<strong>in</strong>g leg to the horizontal<br />

l<strong>in</strong>e θ 1 , the angle of the lower support<strong>in</strong>g leg to the<br />

horizontal l<strong>in</strong>e θ 2 . And it has the maximum value only<br />

when the sum of θ 1 and θ 2 is the largest and s<strong>in</strong>θ 1 is<br />

almost equal to cosθ 2 .<br />

B. FEM Modell<strong>in</strong>g<br />

FEM software is used to simulate and analyze stress<br />

and deformation of the support<strong>in</strong>g mechanism to ensure<br />

the strength and rigidity of the whole robot mechanism.<br />

When the mobile robot arrives at the perforation position,<br />

the electric telescopic rod is power on and the support<strong>in</strong>g<br />

legs are supported onto the pipe wall. The whole robot<br />

mechanism is hovered <strong>in</strong> the oil pipe steadily and the<br />

EDM plug mechanism starts to work. Therefore the<br />

support<strong>in</strong>g mechanism should have enough support<strong>in</strong>g<br />

force to support the whole mechanism. The forces on the<br />

support<strong>in</strong>g mechanism are ma<strong>in</strong>ly the electromagnetic<br />

force, the gravity and the act<strong>in</strong>g force with the pipe wall.<br />

Therefore the electromagnetic force and the gravity can<br />

be simplified to the force acted on the upper and lower<br />

support<strong>in</strong>g plates only.<br />

The f<strong>in</strong>ite element model of the support<strong>in</strong>g mechanism<br />

is established us<strong>in</strong>g the 3-D model<strong>in</strong>g element SOLID98<br />

as shown <strong>in</strong> Fig. 5. The high precision element SOLID98<br />

is adopted to analyze the stress and deformation. It is<br />

1<br />

2<br />

because that the SOLID98 element is a ten nodes<br />

Tetrahedral element and more suitable for produc<strong>in</strong>g the<br />

irregular shape grid [15, 16]. In addition, the guid<strong>in</strong>g rod<br />

is <strong>in</strong>troduced to be analyzed the stress and deformation<br />

based on FEM. The guid<strong>in</strong>g rod is throughout the<br />

support<strong>in</strong>g mechanism (shown <strong>in</strong> Fig. 1 (b)) and places<br />

an important role at the aspect of guid<strong>in</strong>g and support<strong>in</strong>g<br />

the whole robot mechanism. Its strength and rigidity can<br />

ensure the stability of the whole robot mechanism.<br />

Sta<strong>in</strong>less steel and alum<strong>in</strong>ium alloy are considered for<br />

simulation <strong>in</strong> the FEM models because the support<strong>in</strong>g<br />

mechanism is manufactured with sta<strong>in</strong>less steel and the<br />

guid<strong>in</strong>g rod is manufactured with alum<strong>in</strong>ium alloy. The<br />

sta<strong>in</strong>less steel has the merit of high strength and the<br />

alum<strong>in</strong>ium alloy has the merit of light weight [17, 18].<br />

The boundary conditions are fixed on the models and<br />

static analyses are performed <strong>in</strong> sequence <strong>in</strong> order to<br />

obta<strong>in</strong> the analysis results of the stress and deformation of<br />

the components.<br />

Figure 5. FEM model of the support<strong>in</strong>g mechanism<br />

IV. RESULTS AND DISCUSSION<br />

A. Displacement and Stress of the Upper Support<strong>in</strong>g<br />

Plate<br />

The upper support<strong>in</strong>g plate is round and has four<br />

connect<strong>in</strong>g p<strong>in</strong>s with the upper support<strong>in</strong>g legs. And it is<br />

stationary fixed with the electric telescopic rod. So it<br />

manly bears the forces of the upper support<strong>in</strong>g legs when<br />

the support<strong>in</strong>g mechanism is supported on to the pipe<br />

wall. Under the effect of the electromagnetic force and<br />

gravity, the displacement of the upper support<strong>in</strong>g plate is<br />

shown <strong>in</strong> Fig. 6 (a). The maximal deformation emerges at<br />

the connect<strong>in</strong>g po<strong>in</strong>ts with the upper support<strong>in</strong>g legs. This<br />

is ma<strong>in</strong>ly ow<strong>in</strong>g to the weight of the whole mechanism<br />

that ultimately caused the connect<strong>in</strong>g po<strong>in</strong>ts buckled.<br />

Therefore the rigidity of the connect<strong>in</strong>g po<strong>in</strong>ts should be<br />

improved. And the manufacture of the connect<strong>in</strong>g po<strong>in</strong>ts<br />

could adopt the special mach<strong>in</strong><strong>in</strong>g technology or the<br />

material used could be the high strength materials<br />

different from the round support<strong>in</strong>g plate. The stress of<br />

the upper support<strong>in</strong>g plate is shown <strong>in</strong> Fig. 6 (b). It can be<br />

seen that the stress value of the upper support<strong>in</strong>g plate is<br />

very small and the maximum value is only 8.85Mpa,<br />

which only emerges <strong>in</strong> m<strong>in</strong>or places. The stress value is<br />

© 2013 ACADEMY PUBLISHER

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