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Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
DOI: 10.5121/meij.2017.4402 11
DISCOVERY OF LAGRANGIAN EQUATION FOR FLUID
MECHANICS
Shuh Jing Ying
University of South FloridaTampa, Florida, USA
ABSTRACT
This paper is intended to build a connection between dynamics and fluid mechanics. Since Lagrangian
equations are very useful tools in dynamics now it is discovered that it can be also used in fluid mechanics,
so connection can be built through this equation... Here, the lagrangian equation is derived from the
momentum equation in fluid mechanics, and then the equation is applied to three different coordinates,
Cartesian, cylindrical and spherical. Certainly the application of the equation is not limited to these three
different coordinates. This is just for illustration. Many applications are expected.
KEYWORDS
Lagrangian equation, Dynamics and fluid mechanics are connected
1. INTRODUCTION
Fluid mechanics is my major in my graduate study. In my memory when I started to study the
fluid mechanics, I learned a complete set of different equations in fluid mechanics. It seems not
much related with dynamics. Here I hope that I can get some connections between dynamics and
fluid mechanics. In dynamics, Lagrangian equations are very useful tools;many equations are
developed with the use of Lagrangian equation. Now based on the momentum equation in fluid
mechanics, I derived the Lagrangian equation, so I prove that Lagrangian equation can be also
used in fluid mechanics. To simplify the derivation, I started the derivation for incompressible
fluid, so a more general form of Lagrangian equation can be further developed. To illustrate the
use of the equation, some examples are given. Those are especially in very familiar area, so
people can immediately recognize that the equation is working. Momentum equations for inviscid
incompressible fluid in Cartesian, cylindrical and spherical coordinates are chosen for the
illustration.
2. DERIVATION OF LAGRANGIAN EQUATION
In dynamics, especially in the Chapter of Lagrange’s equations, the position vector r is
considered as a function of generalized coordinates q and time t.
r = r(q ,t )
And velocity is a function of generalized coordinatesq , generalized velocity q and time t.
=	 q , q , t
These notations will be used here in this paper.
Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
12
In fluid mechanics, for incompressible fluid, when a portion of fluid is observed, following this
portion of fluid, the momentum equation can be written as
Where 	is	density, 	is	the	substantial	derivative, 	is	velocity	and	 	is	force	per	volume.
Applying the virtual work concept, the equation becomes
Since the virtual work is done at one instant of time, r is function of generalized coordinates only,
so
Now equation (3) is to be considered by two parts, first part is
Since
#
#$%
=	
#
#$%
which is proved in Equation (4 – 12) in Ying’s Advanced Dynamics [1] and
= ,
where T =
&'
(
kinetic energy per unit mass. For the other term
Where Q 	is called generalized force = F․․․․*
*$%
....Hence by combining equations (4) and (5) with (3),
we Have
Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
13
Because all the q+	areindependent, the coefficients must be zero. Therefore,
This is the Lagrangian equation for incompressible fluid in fluid mechanics.
3. APPLICATION
To illustrate the use of the equation three different coordinates are chosen, Cartesian, cylindrical
andspherical. Since they are familiar to everybody, they can be recognized easily.
A. Cartesian Coordinates
Applying the Lagrangian equation
As q = x	, we have
where u = x, v = y, w = z and P is pressure.
Similarly for q = y, we have
For q = z, we have
Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
14
B. CYLINDRICAL COORDINATES
For q = R	,	 we have
For q = 	/ , we have
Since
#
#0
=	12R.
Similarly, for q = z	,	we have
Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
15
Where V4 =	R	, 	V0 = Rφ	, V6 =	zand
C. SPHERICAL COORDINATES
For q = r	,we have
For q = 	θ , we have
Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017
16
Similarly for q = 	φ	,	 we have
whereV8 =	r,			V9 = rθ	, V0 = r	 sin θ	φ	,
4. CONCLUSION
This paper may be considered as the first step for the use of Lagrangian equation in fluid
mechanics. An inviscid incompressible fluid is considered here, more general form of the
Lagrangian equation can be developed for more general kind of fluid. Now the door is open,
further development and application of the equation can be very fruitful to scientists in fluid
mechanics.
REFERENCE
1. Ying, S. J. ‘ Advanced Dynamics ‘ AIAA Education Series 1997.

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DISCOVERY OF LAGRANGIAN EQUATION FOR FLUID MECHANICS

  • 1. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 DOI: 10.5121/meij.2017.4402 11 DISCOVERY OF LAGRANGIAN EQUATION FOR FLUID MECHANICS Shuh Jing Ying University of South FloridaTampa, Florida, USA ABSTRACT This paper is intended to build a connection between dynamics and fluid mechanics. Since Lagrangian equations are very useful tools in dynamics now it is discovered that it can be also used in fluid mechanics, so connection can be built through this equation... Here, the lagrangian equation is derived from the momentum equation in fluid mechanics, and then the equation is applied to three different coordinates, Cartesian, cylindrical and spherical. Certainly the application of the equation is not limited to these three different coordinates. This is just for illustration. Many applications are expected. KEYWORDS Lagrangian equation, Dynamics and fluid mechanics are connected 1. INTRODUCTION Fluid mechanics is my major in my graduate study. In my memory when I started to study the fluid mechanics, I learned a complete set of different equations in fluid mechanics. It seems not much related with dynamics. Here I hope that I can get some connections between dynamics and fluid mechanics. In dynamics, Lagrangian equations are very useful tools;many equations are developed with the use of Lagrangian equation. Now based on the momentum equation in fluid mechanics, I derived the Lagrangian equation, so I prove that Lagrangian equation can be also used in fluid mechanics. To simplify the derivation, I started the derivation for incompressible fluid, so a more general form of Lagrangian equation can be further developed. To illustrate the use of the equation, some examples are given. Those are especially in very familiar area, so people can immediately recognize that the equation is working. Momentum equations for inviscid incompressible fluid in Cartesian, cylindrical and spherical coordinates are chosen for the illustration. 2. DERIVATION OF LAGRANGIAN EQUATION In dynamics, especially in the Chapter of Lagrange’s equations, the position vector r is considered as a function of generalized coordinates q and time t. r = r(q ,t ) And velocity is a function of generalized coordinatesq , generalized velocity q and time t. = q , q , t These notations will be used here in this paper.
  • 2. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 12 In fluid mechanics, for incompressible fluid, when a portion of fluid is observed, following this portion of fluid, the momentum equation can be written as Where is density, is the substantial derivative, is velocity and is force per volume. Applying the virtual work concept, the equation becomes Since the virtual work is done at one instant of time, r is function of generalized coordinates only, so Now equation (3) is to be considered by two parts, first part is Since # #$% = # #$% which is proved in Equation (4 – 12) in Ying’s Advanced Dynamics [1] and = , where T = &' ( kinetic energy per unit mass. For the other term Where Q is called generalized force = F․․․․* *$% ....Hence by combining equations (4) and (5) with (3), we Have
  • 3. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 13 Because all the q+ areindependent, the coefficients must be zero. Therefore, This is the Lagrangian equation for incompressible fluid in fluid mechanics. 3. APPLICATION To illustrate the use of the equation three different coordinates are chosen, Cartesian, cylindrical andspherical. Since they are familiar to everybody, they can be recognized easily. A. Cartesian Coordinates Applying the Lagrangian equation As q = x , we have where u = x, v = y, w = z and P is pressure. Similarly for q = y, we have For q = z, we have
  • 4. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 14 B. CYLINDRICAL COORDINATES For q = R , we have For q = / , we have Since # #0 = 12R. Similarly, for q = z , we have
  • 5. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 15 Where V4 = R , V0 = Rφ , V6 = zand C. SPHERICAL COORDINATES For q = r ,we have For q = θ , we have
  • 6. Mechanical Engineering: An International Journal (MEIJ), Vol. 4, No. 1/2/3/4, November 2017 16 Similarly for q = φ , we have whereV8 = r, V9 = rθ , V0 = r sin θ φ , 4. CONCLUSION This paper may be considered as the first step for the use of Lagrangian equation in fluid mechanics. An inviscid incompressible fluid is considered here, more general form of the Lagrangian equation can be developed for more general kind of fluid. Now the door is open, further development and application of the equation can be very fruitful to scientists in fluid mechanics. REFERENCE 1. Ying, S. J. ‘ Advanced Dynamics ‘ AIAA Education Series 1997.