In the given figure, the particles have charge, \[{{q}_{1}}=-{{q}_{2}}=100nC\text{ }\]\[\text{and }{{q}_{3}}=-{{q}_{4}}=200nC\],and if the distance, \[a=5.0cm\]. What are the x components of force?
                             

Hint: We can find the force due to a combination of static charges by comparing the forces due to each pair of the charges. Here, we are to find the force along the x-component of the setup. We can consider this by taking one of the charges into account.

Complete answer:
We are given four charges arranged in the corners of a square of side ‘a’. We have to find the x-component of electric force due to this arrangement. In order to do that, we have to consider one of the charges on which the forces act due to other charges. We know that taking the charge on the x-axis will make our approach easier.
Let us consider \[{{q}_{3}}\]as the central charge. Now, we can find the force on a charge ‘q’ due to another charge ‘Q’ at distance ‘r’ is given by –
\[{{F}_{e}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{qQ}{{{r}^{2}}}\]
                        
Now, let us consider the given situation of charges.

Let us consider the forces on the charge \[{{q}_{3}}\] due to the other charges using vector algebra –
\[\begin{align}
  & {{F}_{e}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{qQ}{{{r}^{2}}} \\
 & {{\overrightarrow{F}}_{3}}={{\overrightarrow{F}}_{1}}+{{\overrightarrow{F}}_{2}}+{{\overrightarrow{F}}_{4}} \\
 & {{\overrightarrow{F}}_{3}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{1}}{{q}_{3}}}{{{a}^{2}}}(-\widehat{j})+\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{2}}}{{{(\sqrt{2}a)}^{2}}}(\cos {{45}^{0}}i+\sin {{45}^{0}}\widehat{j})+\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{4}}}{{{a}^{2}}}\widehat{i} \\
\end{align}\]
Let us now, consider the x-components of force. All the force components with the vector ‘i’ counts to be the x-components. So, let us group them as –
\[\begin{align}
  & \overrightarrow{{{F}_{3x}}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{2}}}{{{(\sqrt{2}a)}^{2}}}(\cos {{45}^{0}}i)+\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{4}}}{{{a}^{2}}}\widehat{i} \\
 & \Rightarrow \text{ }\overrightarrow{{{F}_{3x}}}=\dfrac{{{q}_{3}}}{4\pi {{\varepsilon }_{0}}}[\dfrac{{{q}_{4}}}{{{a}^{2}}}\widehat{i}+\dfrac{{{q}_{2}}}{{{(\sqrt{2}a)}^{2}}}(\cos {{45}^{0}})] \\
\end{align}\]
Now, we can substitute the values of the charges as given –
\[\begin{align}
  & \overrightarrow{{{F}_{3x}}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{2}}}{{{(\sqrt{2}a)}^{2}}}(\cos {{45}^{0}}i)+\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{q}_{3}}{{q}_{4}}}{{{a}^{2}}}\widehat{i} \\
 & {{q}_{1}}=-{{q}_{2}}=100nC\text{ } \\
 & {{q}_{3}}=-{{q}_{4}}=200nC \\
 & \text{and,} \\
 & a=5.0cm \\
\end{align}\]
\[\begin{align}
  & \Rightarrow \text{ }\left| \overrightarrow{{{F}_{3x}}} \right|=\dfrac{{{q}_{3}}}{4\pi {{\varepsilon }_{0}}}[\dfrac{{{q}_{4}}}{{{a}^{2}}}\widehat{i}+\dfrac{{{q}_{2}}}{{{(\sqrt{2}a)}^{2}}}(\cos {{45}^{0}})] \\
 & \Rightarrow \text{ }\left| \overrightarrow{{{F}_{3x}}} \right|=200\times {{10}^{-9}}\times 9\times {{10}^{9}}[\dfrac{200\times {{10}^{-9}}}{{{(5\times {{10}^{-2}})}^{2}}}+\dfrac{200\times {{10}^{-9}}}{{{(\sqrt{2}\times 5\times {{10}^{-2}})}^{2}}}(\dfrac{1}{\sqrt{2}})] \\
 & \Rightarrow \text{ }\left| \overrightarrow{{{F}_{3x}}} \right|=1800\times [\dfrac{200\times {{10}^{-9}}}{25\times {{10}^{-4}}}+\dfrac{200\times {{10}^{-9}}}{50\sqrt{2}\times {{10}^{-4}}}] \\
 & \Rightarrow \text{ }\left| \overrightarrow{{{F}_{3x}}} \right|=0.19N \\
\end{align}\]
So, the force along the x-axis is approximately 0.2N. This is the required solution for the given data.

Note:
We can either use the vector calculation as we did here, or can consider the signs of the charge while substitution in the formula. You should be careful not to consider the force direction beforehand and again apply the charges in the substitution.