What is the relationship between electric field and charge distribution?

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SUMMARY

The discussion focuses on the electric field generated by a semi-infinite insulating rod with a constant charge per unit length, denoted as λ. It establishes that the electric field at point P makes a 45-degree angle with the rod, and the resultant electric field is expressed as E = √2 (λ / (4 π ε₀ R)). The calculations involve integrating the contributions to the electric field in both the vertical and horizontal directions, confirming that the angle is independent of R, although some participants express uncertainty regarding the convergence of the integrals involved.

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stunner5000pt
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pleas help! electric field

a semi infinite insulting rod carries a constant charge per unit length of lambda. SHow that he electric field at the point P makes an angle of 45 with the rod and that this result is independent of R

[tex]q = \lambda x[/tex]
[tex]dq = \lambda dx[/tex]

for the Y direction poiting downward
[tex]dE_{y} = \int_{0}^{\infty} \frac{1}{4 \pi \epsilon_{0}} \frac{\lambda dx}{R^2 + x^2} \sin{\theta}[/tex]
[tex]\sin{\theta} = \frac{x}{R^2 + x^2}[/tex]
[tex]dE_{y} = \int_{0}^{\infty} \frac{1}{4 \pi \epsilon_{0}} \frac{\lambda R dx}{(R^2 + x^2)^\frac{3}{2}}[/tex]
[tex]dE_{y} = \frac{\lambda R}{4 \pi \epsilon_{0}} \int_{0}^{\infty} \frac{dx}{(R^2 + x^2)^\frac{3}{2}}[/tex]
[tex]dE_{y} = \frac{\lambda R}{4 \pi \epsilon_{0}} [\frac{x}{R^2 \sqrt{R^2+x^2}}]_{0}^{\infty}[/tex]
now I am not sure about this integral and whether or not it converges...

for the horizontal pointing left
[tex]\frac{\lambda R}{4 \pi \epsilon_{0}} \int_{0}^{\infty} \frac{xdx}{(R^2 + x^2)^\frac{3}{2}}[/tex]
same problem here

please help!
 

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stunner5000pt said:
a semi infinite insulting rod carries a constant charge per unit length of lambda. SHow that he electric field at the point P makes an angle of 45 with the rod and that this result is independent of R

[tex]q = \lambda x[/tex]
[tex]dq = \lambda dx[/tex]

for the Y direction poiting downward
[tex]dE_{y} = \int_{0}^{\infty} \frac{1}{4 \pi \epsilon_{0}} \frac{\lambda dx}{R^2 + x^2} \sin{\theta}[/tex]
[tex]\sin{\theta} = \frac{x}{R^2 + x^2}[/tex]
[tex]dE_{y} = \int_{0}^{\infty} \frac{1}{4 \pi \epsilon_{0}} \frac{\lambda R dx}{(R^2 + x^2)^\frac{3}{2}}[/tex]
[tex]dE_{y} = \frac{\lambda R}{4 \pi \epsilon_{0}} \int_{0}^{\infty} \frac{dx}{(R^2 + x^2)^\frac{3}{2}}[/tex]
[tex]dE_{y} = \frac{\lambda R}{4 \pi \epsilon_{0}} [\frac{x}{R^2 \sqrt{R^2+x^2}}]_{0}^{\infty}[/tex]
now I am not sure about this integral and whether or not it converges...

The integral is right and the limit to evaluate is almost trivial: pull x² out of the square root.
 
ok for the Y part
[tex]E_{y} = \frac{\lambda}{4 \pi \epsilon_{0}R}[/tex]
i swhat i got the Y part. Am i right??

for the X part
i got the same thing.
However the resultant for these two given a 45 degree angle... however it isn ot independat of R as in
[tex]E = \sqrt{2} \frac{\lambda}{4 \pi \epsilon_{0}R}[/tex]
 

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