There is a paraboloid in space made by revolving about z axis if the structure extends to infinity having a uniform surface charge density. The co- ordinates of the points on the axis in the concave part of the paraboloid where the electric field vanishes is z=infinity but the potential is infinite at two points i.e. at the vertex and at the focus so there should be at least one point where field is 0 where z<1 but electric field decreases uniformly from the vertex to infinite. This is a paradox worth clarifying. could you please share your views with this.
at z=0 Vis infinity and at z=1 V=infinite but nowhere between[0,1] is the electric field 0
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the following expressions are given for a parabola with surface charge density lamda
The field and potential due to a paraboloid, as described, having surface charge density σ is given by:
E=ϵ0σ∫0∞((z−t)2+4t)3/21+t(z−t)dt,
V=ϵ0σ∫0∞(z−t)2+4t1+tdt
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did you take parametric co-ordinates as (t^2,2t) for a parabola y2=4x
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can you please tell me how to post images
No, t is the vertical height, and z is the height at which electric field and potential is to be found.
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t=x2 in my equation , I don't get yours. Btw, couldn't you cancel π, as the dA term contains π and denominator also contains π as 4πϵ0.
Even if I substituteLog in to reply
y2=4x for convenience we have to find electric field at x=x
Actually i considered only a single parabola of linear charge density consideringE=2∫0∞r2(kλ(ds))cosθ
ds=dx1+(dxdy)2=d(t2)1+(t1)2=2dt1+t2
r=distance(x,0)↔(t2,2t)=(x−t2)2+(2t)2
cosθ=r(x−t2)
E=πεoλ∫0∞((x−t2)2+4t2)3/2dt1+t2(x−t2)
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λ is surface charge density, and you use it as linear charge density. The fields and potentials are due to whole parabaloid, evaluated by cutting rings.
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