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Question: four equal charges of value \[+Q\] are placed at any four vertices of a regular hexagon of side ‘a’....

four equal charges of value +Q+Q are placed at any four vertices of a regular hexagon of side ‘a’. By choosing the vertices, what can be the maximum possible magnitude of the electric field at the centre of the hexagon?
A. Q4πε0a2\dfrac{Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}}
B. 2Q4πε0a2\dfrac{\sqrt{2}Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}}
C. 3Q4πε0a2\dfrac{\sqrt{3}Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}}
D. 2Q4πε0a2\dfrac{2Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}}

Explanation

Solution

-To get maximum possible magnitude of electric field at the centre of hexagon. We arrange four equal charges of value (+Q)\left( +Q \right) in series, then due to two charges, the horizontal component of the electric field is added and the vertical component is canceled out.

Complete step by step answer:
When four charges of magnitude (+Q)\left( +Q \right) are placed in such a way as shown in figure

Let us consider a regular hexagon ABCDEF and four (+Q)\left( +Q \right) charges situated at point A, B, C, and D respectively.
Electric field formula due to a point charge E=14πε0Qr2E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{r}^{2}}}
Where QQ is the charge and rr is the distance between the charge and the point at which the field is found.
All the triangles are equilateral triangles, so the electric field at O due to charge (+Q)\left( +Q \right) at point A.
E1=14πε0Qa2{{E}_{1}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}} ……………………(1)
The electric field at O due to charge (+Q)\left( +Q \right) at point B .
E2=14πε0Qa2{{E}_{2}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}} ……………………….(2)
The electric field at O due to charge (+Q)\left( +Q \right) at point C .
E3=14πε0Qa2{{E}_{3}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}} ……………………………….(3)
The electric field at O due to charge (+Q)\left( +Q \right) at point D .
E4=14πε0Qa2{{E}_{4}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}} ……………………………(4)
From equation (1) and equation (4)
The magnitude of E1{{E}_{1}} and E4{{E}_{4}} are the same but direction is opposite to each other, so the resultant electric field of both are zero.
But from equation (2) and (3)
The magnitude of E2{{E}_{2}} and E3{{E}_{3}} are the same, but its horizontal components are added and the vertical component cancels out.
So resultant electric field is
E=E2cos45+E3cos45E={{E}_{2}}\cos 45{}^\circ +{{E}_{3}}\cos 45{}^\circ
E=14πε0Qa2cos45+14πε0Qa2cos45 E=Q4πε0a2[12+12] E=2Q4πε0a2 \begin{aligned} & E=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}}\cos {{45}^{{}^\circ }}+\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Q}{{{a}^{2}}}\cos 45{}^\circ \\\ & E=\dfrac{Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}}\left[ \dfrac{1}{\sqrt{2}}+\dfrac{1}{\sqrt{2}} \right] \\\ & E=\dfrac{\sqrt{2}Q}{4\pi {{\varepsilon }_{0}}{{a}^{2}}} \\\ \end{aligned}

Note:
When the student calculate the resultant electric field the term cos45 has left many times, so carefully use the formula with all terms