Electric Field of a quarter ring

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SUMMARY

The discussion focuses on calculating the electric field of a quarter ring using the expressions for the electric field components, \(dE_x\) and \(dE_y\). The integration of these components is performed with respect to the angles \(\theta_1\) and \(\theta_2\), which can be set to any values, such as \(\theta_1 = \frac{\pi}{2}\) and \(\theta_2 = \pi\). Despite variations in the limits of integration, the net electric field vector's magnitude and direction remain consistent across different methods. The orientation of the quarter ring significantly influences the resulting electric field components.

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Homework Statement
When calculating electric field of a quarter ring, putting limits from 0 to π/2 gives field lambda/4πER but when I put the limits as -theta1 to theta 2 taking theta from the middle symmetric axis,it gives a different value= lambda/2√2πER. Why does changing limits change the field?
Relevant Equations
dE=Integral kdq/r²
IMG20240624003952.jpg
 
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Define your starting and ending angles conventionally counterclockwise with respect to the positive x-axis as shown in the figure on the right.
Then $$\begin{align} & dE_x=\frac{k\lambda}{R}\cos\theta~d\theta \nonumber \\
& dE_y=\frac{k\lambda }{R}\sin\theta ~d\theta.\nonumber \end{align}$$ Integrate and set the limiting angles ##\theta_1## and ##\theta_2## to whatever you like. One expression does all cases.

For example, in your case I, ##\theta_1=\dfrac{\pi}{2}## and ##\theta_2=\pi.##
 
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Zayan said:
Why does changing limits change the field?
It's not surprising that ##E_x## is different for your two methods. Likewise for ##E_y##.
But your two methods give the same result for the magnitude and direction of the net electric field vector.
 
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kuruman said:
View attachment 347300Define your starting and ending angles conventionally with respect to the positive x-axis as shown in the figure on the right.
Then $$\begin{align} & dE_x=\frac{k\lambda}{R}\cos\theta~d\theta \nonumber \\
& dE_y=\frac{k\lambda }{R}\sin\theta ~d\theta.\nonumber \end{align}$$ Integrate and set the limiting angles ##\theta_1## and ##\theta_2## to whatever you like. One expression does all cases.

For example, in your case I, ##\theta_1=\dfrac{\pi}{2}## and ##\theta_2=\p

TSny said:
It's not surprising that ##E_x## is different for your two methods. Likewise for ##E_y##.
But your two methods give the same result for the magnitude and direction of the net electric field vector.
Yessir it was the Orientation problem
 
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