I Integral equation for large surfaces

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The discussion focuses on the conditions under which terms of a surface integral can be neglected for large surfaces. It is established that the vector field A must approach zero at infinity faster than the surface area grows to justify neglecting these terms. If the decay rate of the field A is slower than the growth rate of the surface, the integral does not equal zero. An example provided is the field of a single point charge, which decreases as 1/r² while the surface area grows as r². This illustrates that the integral remains non-zero under certain conditions.
Apashanka
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We often neglect the terms of a surface integral ##\int_v(\nabla•A)dv=\int_s(A•ds)## for ##s## to be very large or ##v## to be very large,
What is actually the reason behind this to neglect??
 
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The field ##\vec A## is assumed to go to zero at infinity at a rate faster than the rate at which the surface grows.
 
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Orodruin said:
The field ##\vec A## is assumed to go to zero at infinity at a rate faster than the rate at which the surface grows.
Okk got it ...thanks @Orodruin
 
Orodruin said:
The field ##\vec A## is assumed to go to zero at infinity at a rate faster than the rate at which the surface grows.
But if the rate at which the vector field ##A## goes to zero at infinity is slower than the rate at which the surface grows ,then also it would be zero ,isn't it??
 
No. You need the assumption of the field going to zero fast enough. Take the example of the field of a single point charge.
 
Orodruin said:
No. You need the assumption of the field going to zero fast enough. Take the example of the field of a single point charge.
Ok the field decreses as ##\frac{1}{r^2}## and the spherical surface element centered at the point charge grows as ##r^2sin\theta d\theta d\phi##
 
Apashanka said:
Ok the field decreses as ##\frac{1}{r^2}## and the spherical surface element centered at the point charge grows as ##r^2sin\theta d\theta d\phi##
And so the integral is not zero.
 
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