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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 482
On the Generalization of Lami’s Theorem
Himanshu Shekhar
Yamunanagar, Haryana, India
Engineer, Dept. of Mechanical Engineering, Kurukshetra University, Haryana, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - This present paper gives a broad idea of cyclic
nature of the convex polygons having odd number of sidesand
their application in static analysis of mechanical and
structural systems. By using Lami’s Theorem we analyze the
static equilibrium for three forces system but as thenumber of
forces increase it becomes very difficult in analysis, hereinthis
paper Lami’s Theorem is modified and generalized to analyze
the system of forces when in static equilibrium and have
coplanar, concurrent andnon-collinearin natureregardlessof
their number. In this paper also a sufficient condition is
derived for vector/space diagram which helps in determining
that whether the vector/space diagram can transform into
cyclic convex polygon/n-gon ornotand itsapplicationinstatic
analysis.
Key Words: Polygon, Lami’sTheorem,Coplanar,Concurrent,
Non-Collinear, Static equilibrium, Vector/Space diagram.
1. INTRODUCTION
From the past works we know the magnitudes of three
coplanar, concurrent and non-collinear forces, which keeps
an object in static equilibrium, with the angles directly
opposite to the corresponding forces is given by [1]
… (i)
where a, b and c are the magnitude of three coplanar,
concurrent and non-collinear forces, which keep the object
in static equilibrium, and α, β and γ are the angles directly
opposite to the forces A, B and C respectively.
The above theorem is named Lami’s theorem after Bernard
Lami (1640-1715) [2].
In the Lami’s theorem sine rule for triangle’s playanessence
role which says
where a, b, and c are the length of the sides of a triangle, and
θ, φ, and δ are the opposite angles, while 2R is the diameter
of the triangle's circumcircle.
1.1 For 3-gon:
In case of triangles i.e. 3-gon we have sine rule given by
equation (i) [3][4]. It is interesting thatn-gon(itisrequested
to reader to treat polygon as convex polygon wherever term
polygon is used in this paper) havingoddnumberofsides i.e.
for n ϵ odd the sine rule gets the similar form as in case of 3-
gon. For time, in this paper brief calculation for 5-gon and 7-
gon are discuss in detail and the pattern that the sine rule
follows.
1.2 For 5-gon:
Let a 5-gon ABCDE cyclic in nature under circle of radius
R and having sides a, b, c, d, e and angles θ1, θ2, θ3, θ4, and θ5
as shown in figure. Let a line OF⊥BC is drawn and m = ∠BOC.
Then,
Considering the fig. of 5-gon, we have
… (ii)
And from ΔFOC,
Or
… (iii)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 483
From fig. of 5-gon, we have
… (iv)
Using equation (ii), (iii) and (iv), we have
Taking sine on both sides, we get
Similarly,
From all above equations, we get
From above we can conclude for any cyclic 5-gon
1.3 For 7-gon:
Let a 7-gon ABCDEFG, cyclic in nature under a circle of
radius R and having sides a, b, c, d, e, f, g and angles θ1, θ2, θ3,
θ4, θ5, θ6 and θ7 as shown in figure. Join GC. Then,
Considering the fig. of 7-gon, we have
… (v)
And
… (vi)
Adding equation (v) and (vi)
Or
Taking both sides sine, we have
Similarly,
From all above equations, we get
From above we can conclude for any cyclic 7-gon,
In the same way for the higher n-gon’s we obtain the same
pattern i.e. for cyclic polygons when n is odd then
… (vii)
Where ∑θalternate denotes the sum of all alternate angles in a
n-gon except the angles associated with the corresponding
side. For e.g. in case of 5-gon ∑θalternate = θ1+θ4 for the side b
and θ2, θ3 are the angles associated with b therefore didn’t
take part in ∑θalternate for the side b.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 484
2. TRANSFORMATION OF n-gon’s INTO VECTOR
DIAGRAM AND VICE VERSA
Any n-gon can be transformed into the vector/space
diagram such that length of the sides of n-gon represents
magnitude of the vectors and the direction of these vectors
from each other can be represent as function of interior
angles of n-gon’s.
Transformation of n-gon intovector diagramcanbedone
by drawing lines (of same magnitude as of sides) parallel to
the sides of the n-gon and bringing thematoneofthevertices
of the n-gon (any vertices can be taken as origin forn-gon for
vector diagram transformation, there be only change in the
transformation matrix with change of vertices) such that the
transformation is optimum and wide to application.
For the time the transformationof3-gon,5-gonand7-gon
is presented but it is true and can be manipulated for any n-
gon.
2.1 For 3-gon:
Transformation can be done by drawing the linesparallel
to the side of the 3-gon and bringing all the sides at one
vertices/point. In the below example of ΔABC having sides a,
b, c corresponding to angles θ1, θ2, θ3 (or A, B, C) respectively,
point B is taken as origin O. These are the steps involved in
the transformation,
1. Point B is set as origin O.
2. Line parallel to b is bring at point B such that it
makes angle α with c.
3. Line parallel to a is bring at point B such that it
makes angles β and γ with c and b respectively as shown in
diagram.
The line parallel to a is drawn here considering the
optimum transformation and having wide to application.
It is easy to obtain from the diagram that the
transformation of 3-gon to vector diagram andviceversacan
be given by
2.2 For 5-gon:
In case of 5-gon ABCDE, point A is taken as origin and
vector transformation of 5-gon is done as shown in diagram.
One can obtain in this case that transformation can be
given by
2.3 For 7-gon:
In case of 7-gon ABCDEFG, point A is againtakenasorigin
and vector transformation of 7-gon is done as shown in
diagram.
In this case transformation can be given by
3. CONDITION FOR THE VECTOR/SPACE DIAGRAM
TO BE CYCLIC n-gon
Let Sn(x) denotes the function of angles and defined as,
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 485
where α, β, γ, θ, δ, … denotes the angles corresponding tothe
vector/space diagram of n-gon. Then,
For 3-gon:
For 5-gon:
In the same way Sn(x) can be obtained for all n-gon.
Equation (vii) in terms of Sn(x) can be given as follow:
… (viii)
To obtain the condition that the vector diagram is cyclic n-
gon or not static analysis relating the co-planar, concurrent
and co-linear vectors are being use.
Consider n-gon vector diagram having vectors of magnitude
a, b, c, d, e, …, n and transformed angles be α, β, γ, θ, δ, …, δn
as considered in vector diagram.
Considering the system is in static equilibrium under vector
a , e , d , b , …, n and c . Let R be the resultant vector of
vectors a , e , d , b , …, n having magnitude R and
countering the vector c .
Therefore, if the system is in static equilibrium then
magnitude of R and c must be same i.e.
… (ix)
The magnitude of resultant vector R can be given by
Where,
From equation (viii) we have,
Where k is some constant.
Putting this value in equation defining R, we get
from equation (ix), we have
Or
Or
Above relation is the required condition for a vector/space
diagram to be cyclic n-gon.
4. CONCLUSIONS
In statics, Lamis’s Theorem is an equation relating the
magnitudes of three co-planar,concurrentandnon-collinear
forces, which keeps an object in static equilibrium with the
angles directly opposite to the corresponding sides.
The Lami’s Theorem can be modified for more than three
forces without hindering its beauty and in more details.Also
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 486
the transformation of n-gon to vector diagram acts like the
bridge which helps in establishing the relationship.
The statements for the generalized Lami’s Theorem can be
given as,
“When three or more than three (number of forces be odd)
co-planar, concurrent and non-collinear forces acts on an
object such that it keeps the object in static equilibrium and
the forces follow the cyclic condition then each forces are
proportional to the sine of thefunctionofanglesbetween the
others forces.” According to theorem,
If
Then for all n belongs odd
REFERENCES
[1] Dubey, N.H. (2013). Engineering Mechanics: Statics and
Dynamics. Tata McGraw-Hill Education.
ISBN 9780071072595
[2] “Lami’s Theorem – Oxford Reference”
[3] R.B. Kershner, “The Law Of Sines And Cosines For
Polygons,” Mathematics Magazine.
DOI: 10.2307/2688227
[4] https://en.wikipedia.org/wiki/Polygon

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IRJET- On the Generalization of Lami’s Theorem

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 482 On the Generalization of Lami’s Theorem Himanshu Shekhar Yamunanagar, Haryana, India Engineer, Dept. of Mechanical Engineering, Kurukshetra University, Haryana, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - This present paper gives a broad idea of cyclic nature of the convex polygons having odd number of sidesand their application in static analysis of mechanical and structural systems. By using Lami’s Theorem we analyze the static equilibrium for three forces system but as thenumber of forces increase it becomes very difficult in analysis, hereinthis paper Lami’s Theorem is modified and generalized to analyze the system of forces when in static equilibrium and have coplanar, concurrent andnon-collinearin natureregardlessof their number. In this paper also a sufficient condition is derived for vector/space diagram which helps in determining that whether the vector/space diagram can transform into cyclic convex polygon/n-gon ornotand itsapplicationinstatic analysis. Key Words: Polygon, Lami’sTheorem,Coplanar,Concurrent, Non-Collinear, Static equilibrium, Vector/Space diagram. 1. INTRODUCTION From the past works we know the magnitudes of three coplanar, concurrent and non-collinear forces, which keeps an object in static equilibrium, with the angles directly opposite to the corresponding forces is given by [1] … (i) where a, b and c are the magnitude of three coplanar, concurrent and non-collinear forces, which keep the object in static equilibrium, and α, β and γ are the angles directly opposite to the forces A, B and C respectively. The above theorem is named Lami’s theorem after Bernard Lami (1640-1715) [2]. In the Lami’s theorem sine rule for triangle’s playanessence role which says where a, b, and c are the length of the sides of a triangle, and θ, φ, and δ are the opposite angles, while 2R is the diameter of the triangle's circumcircle. 1.1 For 3-gon: In case of triangles i.e. 3-gon we have sine rule given by equation (i) [3][4]. It is interesting thatn-gon(itisrequested to reader to treat polygon as convex polygon wherever term polygon is used in this paper) havingoddnumberofsides i.e. for n ϵ odd the sine rule gets the similar form as in case of 3- gon. For time, in this paper brief calculation for 5-gon and 7- gon are discuss in detail and the pattern that the sine rule follows. 1.2 For 5-gon: Let a 5-gon ABCDE cyclic in nature under circle of radius R and having sides a, b, c, d, e and angles θ1, θ2, θ3, θ4, and θ5 as shown in figure. Let a line OF⊥BC is drawn and m = ∠BOC. Then, Considering the fig. of 5-gon, we have … (ii) And from ΔFOC, Or … (iii)
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 483 From fig. of 5-gon, we have … (iv) Using equation (ii), (iii) and (iv), we have Taking sine on both sides, we get Similarly, From all above equations, we get From above we can conclude for any cyclic 5-gon 1.3 For 7-gon: Let a 7-gon ABCDEFG, cyclic in nature under a circle of radius R and having sides a, b, c, d, e, f, g and angles θ1, θ2, θ3, θ4, θ5, θ6 and θ7 as shown in figure. Join GC. Then, Considering the fig. of 7-gon, we have … (v) And … (vi) Adding equation (v) and (vi) Or Taking both sides sine, we have Similarly, From all above equations, we get From above we can conclude for any cyclic 7-gon, In the same way for the higher n-gon’s we obtain the same pattern i.e. for cyclic polygons when n is odd then … (vii) Where ∑θalternate denotes the sum of all alternate angles in a n-gon except the angles associated with the corresponding side. For e.g. in case of 5-gon ∑θalternate = θ1+θ4 for the side b and θ2, θ3 are the angles associated with b therefore didn’t take part in ∑θalternate for the side b.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 484 2. TRANSFORMATION OF n-gon’s INTO VECTOR DIAGRAM AND VICE VERSA Any n-gon can be transformed into the vector/space diagram such that length of the sides of n-gon represents magnitude of the vectors and the direction of these vectors from each other can be represent as function of interior angles of n-gon’s. Transformation of n-gon intovector diagramcanbedone by drawing lines (of same magnitude as of sides) parallel to the sides of the n-gon and bringing thematoneofthevertices of the n-gon (any vertices can be taken as origin forn-gon for vector diagram transformation, there be only change in the transformation matrix with change of vertices) such that the transformation is optimum and wide to application. For the time the transformationof3-gon,5-gonand7-gon is presented but it is true and can be manipulated for any n- gon. 2.1 For 3-gon: Transformation can be done by drawing the linesparallel to the side of the 3-gon and bringing all the sides at one vertices/point. In the below example of ΔABC having sides a, b, c corresponding to angles θ1, θ2, θ3 (or A, B, C) respectively, point B is taken as origin O. These are the steps involved in the transformation, 1. Point B is set as origin O. 2. Line parallel to b is bring at point B such that it makes angle α with c. 3. Line parallel to a is bring at point B such that it makes angles β and γ with c and b respectively as shown in diagram. The line parallel to a is drawn here considering the optimum transformation and having wide to application. It is easy to obtain from the diagram that the transformation of 3-gon to vector diagram andviceversacan be given by 2.2 For 5-gon: In case of 5-gon ABCDE, point A is taken as origin and vector transformation of 5-gon is done as shown in diagram. One can obtain in this case that transformation can be given by 2.3 For 7-gon: In case of 7-gon ABCDEFG, point A is againtakenasorigin and vector transformation of 7-gon is done as shown in diagram. In this case transformation can be given by 3. CONDITION FOR THE VECTOR/SPACE DIAGRAM TO BE CYCLIC n-gon Let Sn(x) denotes the function of angles and defined as,
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 485 where α, β, γ, θ, δ, … denotes the angles corresponding tothe vector/space diagram of n-gon. Then, For 3-gon: For 5-gon: In the same way Sn(x) can be obtained for all n-gon. Equation (vii) in terms of Sn(x) can be given as follow: … (viii) To obtain the condition that the vector diagram is cyclic n- gon or not static analysis relating the co-planar, concurrent and co-linear vectors are being use. Consider n-gon vector diagram having vectors of magnitude a, b, c, d, e, …, n and transformed angles be α, β, γ, θ, δ, …, δn as considered in vector diagram. Considering the system is in static equilibrium under vector a , e , d , b , …, n and c . Let R be the resultant vector of vectors a , e , d , b , …, n having magnitude R and countering the vector c . Therefore, if the system is in static equilibrium then magnitude of R and c must be same i.e. … (ix) The magnitude of resultant vector R can be given by Where, From equation (viii) we have, Where k is some constant. Putting this value in equation defining R, we get from equation (ix), we have Or Or Above relation is the required condition for a vector/space diagram to be cyclic n-gon. 4. CONCLUSIONS In statics, Lamis’s Theorem is an equation relating the magnitudes of three co-planar,concurrentandnon-collinear forces, which keeps an object in static equilibrium with the angles directly opposite to the corresponding sides. The Lami’s Theorem can be modified for more than three forces without hindering its beauty and in more details.Also
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 10 | Oct 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 486 the transformation of n-gon to vector diagram acts like the bridge which helps in establishing the relationship. The statements for the generalized Lami’s Theorem can be given as, “When three or more than three (number of forces be odd) co-planar, concurrent and non-collinear forces acts on an object such that it keeps the object in static equilibrium and the forces follow the cyclic condition then each forces are proportional to the sine of thefunctionofanglesbetween the others forces.” According to theorem, If Then for all n belongs odd REFERENCES [1] Dubey, N.H. (2013). Engineering Mechanics: Statics and Dynamics. Tata McGraw-Hill Education. ISBN 9780071072595 [2] “Lami’s Theorem – Oxford Reference” [3] R.B. Kershner, “The Law Of Sines And Cosines For Polygons,” Mathematics Magazine. DOI: 10.2307/2688227 [4] https://en.wikipedia.org/wiki/Polygon