Definite integral on elliptic integral where modulus is function of variable

Rh \tan \theta}{(R+h \tan \theta)^2+Z^2}} $.In summary, we are trying to prove the identity $\int_{0}^{\frac{\pi }{2}}{\sqrt {\sin \theta cos\theta}k(\theta) K[k(\theta)]}d\theta=\pi \sqrt{ \frac{Rh}{R^2 + (h+Z)^2}} $, where $ k(\theta)=\sqrt\frac{4Rh \tan \theta}{Z^2+(R+h \tan \theta)^2} $ and $ K[k(\theta)] $ is
  • #1
bshoor
5
1
How to prove:

$\int_{0}^{\frac{\pi }{2}} {\frac{\sin \theta}{\sqrt{Z^2+(R+h \tan \theta)^2}} K[k(\theta)]}=\frac{\pi }{2\sqrt{R^2 + (h+Z)^2}} $

where \[ k(\theta)=\sqrt\frac{4Rh \tan \theta}{Z^2+(R+h \tan \theta)^2}\]

and $ K[k(\theta)] $ is the complete elliptic integral of the first kind, defined by

\[ K[k(\theta)]= \int_0^{\frac{\pi }{2}}\frac{\,d\phi}{\sqrt{1-k^2(\theta)\sin^2 \phi}}\]

and h, R and Z $ \gt 0 $
 
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  • #2
Can you show us what you have tried and where you are stuck? This will give our helpers a better idea how to provide help without perhaps offering suggestions that you may already be trying.
 
  • #3
bshoor said:
How to prove:

$\int_{0}^{\frac{\pi }{2}} {\frac{\sin \theta}{\sqrt{Z^2+(R+h \tan \theta)^2}} K[k(\theta)]}=\frac{\pi }{2\sqrt{R^2 + (h+Z)^2}} $

where \[ k(\theta)=\sqrt\frac{4Rh \tan \theta}{Z^2+(R+h \tan \theta)^2}\]

and $ K[k(\theta)] $ is the complete elliptic integral of the first kind, defined by

\[ K[k(\theta)]= \int_0^{\frac{\pi }{2}}\frac{\,d\phi}{\sqrt{1-k^2(\theta)\sin^2 \phi}}\]

and h, R and Z $ \gt 0 $
Please make correction of the post:
$\int_{0}^{\frac{\pi }{2}} {\frac{\sin \theta}{\sqrt{Z^2+(R+h \tan \theta)^2}} K[k(\theta)]}d\theta=\frac{\pi }{2\sqrt{R^2 + (h+Z)^2}} $
 
  • #4
MarkFL said:
Can you show us what you have tried and where you are stuck? This will give our helpers a better idea how to provide help without perhaps offering suggestions that you may already be trying.

I have tried in different ways. But the integral becomes more and more complicated. Anyway the identity can be modified to :

$\int_{0}^{\frac{\pi }{2}}{\sqrt {\sin \theta cos\theta}k(\theta) K[k(\theta)]}d\theta=\pi \sqrt{ \frac{Rh}{R^2 + (h+Z)^2}} $

by multiplying both side by $ 2 \sqrt{Rh} $
 

FAQ: Definite integral on elliptic integral where modulus is function of variable

What is a definite integral on an elliptic integral?

A definite integral on an elliptic integral is a mathematical operation that combines the concepts of definite integration and elliptic integrals. It involves finding the area under a curve that represents an elliptic function, where the limits of integration are defined by the values of the modulus, which is a function of a variable.

What is an elliptic integral?

An elliptic integral is a type of integral that involves integrating an elliptic function, which is a special type of function that has real or complex variables. It is used to solve many problems in physics, engineering, and mathematics, and has many applications in fields such as celestial mechanics, electromagnetism, and quantum mechanics.

How does the modulus affect the definite integral on an elliptic integral?

The modulus is a key parameter in elliptic integrals, and it determines the shape of the elliptic function and the behavior of the definite integral. As the modulus varies, the limits of integration and the resulting area under the curve also change. This means that the value of the definite integral will be different for different values of the modulus.

What is the significance of using a variable modulus in the definite integral on an elliptic integral?

Using a variable modulus in the definite integral on an elliptic integral allows for a more flexible and versatile approach to solving problems. It allows the integration to be applied to a wider range of functions, and it enables the solution to be generalized for different values of the modulus. This makes it a powerful tool in many areas of mathematics and science.

How is the definite integral on an elliptic integral used in real-world applications?

The definite integral on an elliptic integral has many real-world applications, including in physics, engineering, and economics. It is used to solve problems involving periodic motion, such as the motion of planets and satellites, and it is also used in the calculation of electric potential and magnetic fields. Additionally, it has applications in the evaluation of financial options and in the study of fluid dynamics.

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