Electric field created by point charges

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SUMMARY

The discussion centers on the electric field generated by point charges arranged in a square configuration. The participants confirm that the contributions from two identical positive charges (2q) cancel each other out at the center, leaving only the effect of a negative charge (-Q). The derived electric field at the center (0,0) is expressed as $$\vec{E}(0,0)=-\frac{\sqrt{2}Qk}{d^2}(1,1)$$, indicating that the field's direction and magnitude depend solely on the negative charge. The participants also clarify that replacing -Q with +Q in the opposite corner yields the same field characteristics, affirming the symmetry in electric fields.

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darioslc
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Homework Statement
Find the electric field in the center of square, if in his three vertices there are three puntual charges:
2q, 2q and Q and the side is d:

2q *-------------
| |
| |
Q *-------------* 2q
Relevant Equations
The only relevant equation is $$E=\frac{kq}{r^2}$$
Hello, I reasoned by simmetry, the two charges with value 2q not contributed at field because there are equidistant at point and are similar charges. Therefor only survival the field due to Q, using the definition for electric field of the puntual charge:
$$\vec{E}(0,0)=-\frac{\sqrt{2}Qk}{d^2}\hat{x}-\frac{\sqrt{2}Qk}{d^2}\hat{y}$$
because I set the square in the center, then:
\begin{align}
E(x,y)=&-\frac{Qk}{[(x+d/2)^2+(y+d/2)^2]^{3/2}}(x+d/2,y+d/2)\text{ evaluated in the (0,0)}\\
E(0,0)=&-\frac{Qk}{[(d/2)^2+(d/2)^2]^{3/2}}(d/2,d/2)\nonumber\\
E(0,0)=&-\frac{Qk}{[2(d/2)^2]^{3/2}}(d/2,d/2)\nonumber\\
E(0,0)=&-\frac{Qk}{[d^2/2]^{3/2}}(d/2,d/2)\nonumber\\
E(0,0)=&-\frac{\sqrt{2}Qk}{d^2}(1,1)\nonumber
\end{align}
which makes senses, because Q is negative.

¿That is correct? because I doubt a little bit
 
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When we put charge Q on the absent corner, center E is obviously zero.
2409201.png

The configuration of single charge -Q as shown below should give same center E we want.
2409202.png

This is my estimation. Does it show same result as yours ?
 
I agree that the contributions of the two charges ##q## cancel each other. This leaves the contribution from charge ##Q## at the lower left corner. The general expression for the electric field at position ##\mathbf r## due to charge ##Q## at position ##\mathbf r'## is $$\mathbf E=kQ\frac{(\mathbf r-\mathbf r')}{|\mathbf r-\mathbf r'|^3}.$$ If you put the origin of coordinates at the center of the square, ##\mathbf r=0##. What is ##\mathbf r'## in this case? What do you get when you substitute in the general expression?
 
anuttarasammyak said:
When we put charge Q on the absent corner, center E is obviously zero.
View attachment 351358
The configuration of single charge -Q as shown below should give same center E we want.
View attachment 351359
This is my estimation. Does it show same result as yours ?
But when you put the charge -Q in the opposite corner (when in original scheme it's absent charge), the field is the same but not the sense, no?
The scheme with the center (0,0) is:
2q *-----------------
| |
| (0,0) |
| |
-Q *----------------* 2q

Excuse me, I see that the sign of Q is -Q, not +Q like in the initial. Anyway, the field value is correct using -Q.
Now I see your reasoning.

Then finally the field due both 2q is zero in the center, except for -Q
 
darioslc said:
But when you put the charge -Q in the opposite corner (when in original scheme it's absent charge), the field is the same but not the sense, no?
No. Charge ##+Q## at the lower left corner produces exactly the same field (magnitude and direction) as charge ##-Q## at the upper right corner.
 
kuruman said:
No. Charge ##+Q## at the lower left corner produces exactly the same field (magnitude and direction) as charge ##-Q## at the upper right corner.
… at the center of the square.

May seem like nitpicking but an important point to note.
 
Orodruin said:
… at the center of the square.

May seem like nitpicking but an important point to note.
Of course.
 

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