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Stoke's theorem. Topics of discussion History Definition of Stoke’s Theorem Mathematical expression Proof of theorem Physical significance Practical applications.

Presentation on theme: "Stoke's theorem. Topics of discussion History Definition of Stoke’s Theorem Mathematical expression Proof of theorem Physical significance Practical applications."— Presentation transcript:

Stoke's theorem

Topics of discussion History Definition of Stoke’s Theorem Mathematical expression Proof of theorem Physical significance Practical applications of Stoke’s Theorem.

STOKES ’ THEOREM The theorem is named after the Irish mathematical physicist Sir George Stokes (1819 – 1903). –What we call Stokes ’ Theorem was actually discovered by the Scottish physicist Sir William Thomson (1824 – 1907, known as Lord Kelvin). –Stokes learned of it in a letter from Thomson in 1850.

Statement of Stoke’s Theorem It states that line integral of a vector field A round any close curve C is equal to the surface integral of the normal component of curl of vector A over an unclosed surface ‘S’.

Mathematical expression A. dr= (X A).dS Stoke’s theorem thus converts surface integral in to a line integral over any path which constitutes the boundary of the surface. C S

where is known as Del Operator It is treated as a vector in Cartesian coordinate system but it has no meaning unless it is operated upon a scalar or vector. It is given by =î∂/∂x+ ĵ∂/∂y+ ^∂/∂z k

X Y Z ∆ s 1 = k ∆s 1 ^ ^ A dr c o

Proof of theorem In order to prove this theorem, we consider that surface ‘S’ is divided in to infinitesimally small surface elements ∆S1,∆S2,∆S3…..etc, having boundaries C1,C2,C3…etc. Boundary of each element is traced out anti-clock wise. x y z c A ∆S 1 =k∆S 1 ^

The line integral of a vector field A round the boundary of a unit area in x-y plane is equal to the component of curl A along positive z-direction. Thus the line integral of a vector field A along the boundary of ith surface is equal to the product of the curl A and normal component of area ∆S i i.e. ∫A.dr =(Curl A). k∆S i = ( X A).k∆S i ^ ^ c A similar process is applied to the surface element,tracing them all in the same sense then above equation holds good for each surface element and if we add all such equations,we have ∑∫ A.dr=∑( X A).K∆S ii...........(1) i=1 n n

Then all the integrals within the interior of surface cancel, because the two integrals are in opposite directions along the common side between two adjacent area elements. The only portions of the line integrals that are left are those along the sides which lie on the boundary C.

Lt ∑(. A).k∆S I = ∫∫(X A). kdS N∞ SiSi 0 i=1 N s ^ ^ Then equation can be written as Hence the equations(1)reduces to ∫A.dr=∫∫( XA).kdS ^ c This is the Stoke’s Theorem for a plane surface.

Physical significance If ∫ A.dl =0 for any closed path, then A is called irrotational or conservative field. If A denotes the force F then ∫F.dr=0 means that total work done by the force in taking a body round a closed curve is zero i.e total energy remains conserved throughout the motion.

Practical applications It is used for determining whether a vector field is conservative or not. It allows one to interpret the curl of vector field as measure of swirling about an axis.

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