Math Physics: Kronecker Delta Fn in Cylindrical/Spherical Polar Coords

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SUMMARY

The discussion focuses on the application of the Kronecker delta function in cylindrical and spherical polar coordinates, clarifying its distinction from the Dirac delta function, which is applicable to continuous variables. The relationship between delta functions and variable transformations is emphasized, particularly how the measure changes across coordinate systems. Key equations are presented, demonstrating the integration of functions involving delta functions and the use of Jacobian determinants in multi-dimensional contexts.

PREREQUISITES
  • Understanding of Kronecker delta function and its application in discrete variables.
  • Familiarity with Dirac delta function and its properties in continuous variables.
  • Knowledge of variable substitution techniques in calculus.
  • Basic understanding of Jacobian determinants in multivariable calculus.
NEXT STEPS
  • Study the properties of the Dirac delta function in various coordinate systems.
  • Explore variable substitution techniques in integration, particularly in relation to delta functions.
  • Learn about Jacobian determinants and their applications in coordinate transformations.
  • Investigate the applications of delta functions in physics, especially in quantum mechanics and field theory.
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Students and professionals in mathematics and physics, particularly those focusing on theoretical physics, calculus, and coordinate transformations in multivariable contexts.

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What will be Kronecker Delta Function in Cylindrical co-ordinates as well as in spherical Polar coordinates?
 
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Do you mean Dirac delta function? The Kronecker delta function is for discrete variables.

That having been said you can view the Dirac delta function as the derivative of a step function (in one variable). In many variables you take products of delta functions for each coordinate. You then must consider how the measure changes in different coordinate systems.

Delta functions of general functions of the variable behave as follows.
Let [itex]u = u(x)[/itex] be a continuous function of x with [itex]u(a)=b[/itex] and [itex]u'(a) \ne 0[/tex].<br /> <br /> Then:<br /> [tex]\int f(x) \delta(u(x)-b)dx = \int f(x)\delta(u-b)\frac{du}{u'} = \frac{f(x)}{u'}|_{u=b}[/tex]<br /> where we use variable substitution: [itex]u=u(x), du = u'dx, dx = du/u'[/itex].<br /> <br /> Since the equation:<br /> [tex]\int f(x)\delta(u(x)-b)dx = \frac{f(a)}{u'(a)}=\int f(x)\frac{\delta(x-a)}{u'(a)}dx[\tex]<br /> holds for arbitrary function [itex]f(x)[/itex][/tex][itex]we have that:<br /> [tex]\delta(u(x)-b) = \frac{1}{u'(a)}\delta(x-a)[/tex]<br /> where<br /> [tex]u(a) = b[/tex]<br /> or equivalently:<br /> [tex]\delta(x-a) = u'(a)\delta(u(x)-u(a))[/tex]<br /> <br /> Similarly if you promote x and u to coordinate vectors and work out the same argument you get:<br /> [tex]\delta^n(\vec{x}-\vec{a}) = \left|\frac{\partial \vec{u}}{\partial \vec{x}}\right|_{\vec{x}=\vec{a}}\delta(\vec{u}(\vec{x})-\vec{u}(\vec{a})[/tex]<br /> where<br /> [tex]\left|\frac{\partial \vec{u}}{\partial \vec{x}}\right|_{\vec{x}=\vec{a}}[/tex]<br /> is the Jacobian determinant at [itex]\vec{a}[/tex] (and n is the dimension.)[/itex][/itex][/itex]
 

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