International Journal of Engineering Trends and Technology (IJETT) – Volume 32 Number 3- February 2016 Study of Paucellier Mechanism Dr. Ali Hasan Mechanical Engineering Department, Jamia Millia Islamia, New Delhi. Abstract –in this paper, the author presented the geometry point A moves in a circular path and as the design procedure of shaper mechanism using point A moves in a circle point P traverses an exact Peaucellier linkage. The been straight line path normal to the line joining O2 and formulated between the angles O4. From the construction of the Peaucellier linkage subtended by the linkages in the Paucellier it is clear that this is a much more complex Mechanism during its motion in shaper mechanism. mechanism The stroke length has been calculated and a generating approximate straight lines, which were relationship has been shown among different simple four bar linkages. This mechanism has eight variables. a prototype also has been tested. members and six joints. relation lengths has and than the mechanisms 1) Key Words- mechanism, height of mechanism and stroke length 2) Introduction: The Paucellier linkage was invented in 1864.It is named after Charles-Nicolas Paucellier (1832–1913), a French army officer. It was the first planar linkage capable of transforming perfect straight-line motion, rotary and motion vice into versa. Paucellier mechanism is one of the exact straight line motion mechanism .It works on lower pair linkages implying eight links rhomboidal system in such a way so as to produce straight line motion at its output. Paucellier mechanism can convert an input circular motion to the exact straight line motion. The construction of this mechanism is such Design Procedure A Mathematical model of paucellier mechanism is shown in Figure 2. that the point which is connected to the crank moves in a circular path and the point traversing the straight line is selected as the output point. The linkage has a rhombic loop formed of the equal length members, 5, 6, 7 and 8 as shown in Figure 1. Two equal length links are connected to the opposite corners of the rhombus at one end and to a common fixed point at the other ends. The point A of the rhombus is connected to a fixed point O2 through the link 2. The length of the link 2 is equal to the distance Mathematical model of paucellier mechanism between points O2 and O4. By the constraints of the ISSN: 2231-5381 http://www.ijettjournal.org Page 132 International Journal of Engineering Trends and Technology (IJETT) – Volume 32 Number 3- February 2016 (i).It consists of 8 links i.e. a fixed link OO1 and the straight links O1A, OC, OD, AD, DB, BC and CA are connected by turning pairs. (ii)The pin at A is constrained to move along the circumference of a circle. (iii) AC = CB = BD = DA; OC = OD; and OO1 = O1A (iv)From the triangles ORC and BRC, (v)Therefore the product OB X OA remains constant. Hence the point B traces a straight path perpendicular to the diameter OP. (OC)2 = (OR)2 + (RC)2 ------------------------------(1) and (BC)2 = (RB)2 + (RC)2 --------------------------------(2) Subtracting equation (2)from (1), we get (OC)2 - (BC)2 = (OR)2 - (RB)2 = (OR+OB) (OROB) = OB X OA Assumptions:- (i) Values of w and h are to be assumed. (ii) l = (h/3) , (iii) d = 2w Here, w is the width of the bar, l is the horizontal length of the mechanism, h is the vertical height of the mechanism, r is the length of the crank bar, lb is the length of each bar of rhomboidal system, lr is the length of rod joining bars of rhomboidal system to the fixed point, d is the vertical height of the rhomboidal system, 2θ is the angle subtended between the rods joining bars of rhomboidal system to the fixed point, See Figure 3 and Figure 4. 2r = h-d In ∆ABD, Tan θ = (AD/BD) ,Tan θ = {(l/2)/h} , or Ɵ= Tan-1{(l/2)/h} In ∆BHF, HB = 2r + (d/2), Tan θ = (FH/HB) or FH = HB × Tan θ FH = {2r + (d/2)} Tan θ In ∆FHE, HE = d/2 ,Tan α = (HE/ FH) , or Tan α = {(d/2) / (2r + (d/2)) Tan θ} Sin α = (HE/FE) , or FE = (HE/ Sin α) , {FE = lb., HE = (d/2)} lb. = {(d/2)/ Sin α} Sin θ = (FH/FB) or Sin θ = {(2r + (d/2)) Tan θ/ lr} lr = {(2r + (d/2)) Tan θ/ Sin θ} or lr = {(2r + (d/2))/ Cos θ} (L/2) = h Tan γ or L = 2h Tan γ. Results: Results are shown in Table-1,2 and 3. ISSN: 2231-5381 http://www.ijettjournal.org Page 133 International Journal of Engineering Trends and Technology (IJETT) – Volume 32 Number 3- February 2016 CASE 2:- h is kept constant and Wmin is varied h= 1200 mm Contants:- h, wmax , d ,θ, lb , lr . Variables:- W‟, Ф, β ,ls ,γ ,L . Quantity on which effect to be noted:- L h= 1200 mm constant , W= 150 mm. CONCLUSION This paper is about formulating the relations between the lengths and angles subtended by the linkages of a paucellier mechanism. The main aim of this paper is to provide a design procedure for the advancement of a shaper mechanism so as to minimizing the errors during manufacturing and working of the mechanism and to avoid the hit and trial method for determining the various lengths and angles of the mechanism. In this paper few relations are deduced to calculate the working angle and by knowing the working angle, one can easily program the motor power to op ISSN: 2231-5381 http://www.ijettjournal.org Page 134 International Journal of Engineering Trends and Technology (IJETT) – Volume 32 Number 3- February 2016 References 1.[Erdman and Sandor, 1988] Erdman A. G. and Sandor G. N., “Advanced Mechanism Design”, Vol. I and II, Prentice Hall of India. 2.[Ghosh and Mallik, 1988] Amitabha Ghosh and Ashok Kumar Mallik, “Theory of Mechanisms and Machines”, East – West Press Pvt. Ltd., New Delhi, pp. II Edition. 3. 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