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In this question we will consider the electric field of a charged rod of length \(L\) at a point \(P\) located a distance \(b\) from the center of the rod along its perpendicular bisector, as illustrated in Figure \(1 .\)
It can be shown that the magnitude of the electric field at \(P(0, b)\) is given by the following integral
$$ E(b)=\int_{-\frac{L}{2}}^{\frac{L}{2}} \frac{\lambda b}{4 \pi \varepsilon_{0}\left(x^{2}+b^{2}\right)^{3 / 2}} d x $$
where \(\lambda\) is the charge density per unit length on the rod and \(\varepsilon_{0}\) is called the permittivity of free space (it is a universal constant with the value \(8.854 \times 10^{-12} \mathrm{~F} / \mathrm{m}\) (farads per metre)).
Where λ is the charge density per unit length on the rod and εο is called the permittivity of fre...
where λ is the charge density per unit length on the rod and εο is called the permittivity of free space (it is a universal constant with the value 8.854 x 10-12 F/m (farads per metre)) The integral for the electric field can be evaluated exactly using a method called trigonometric substitution with the result AL We won't learn the method of trigonometric substitution in this course; however, you will approximate the value of the integral using methods we introduced...
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