Electrostatic Energy of Square Charge Configuration
Example
Question:
    Four charges are arranged at the corners of a square \(ABCD\) of side \(d\), as shown in Fig. 2.15(a).
    (a) Find the work required to put together this arrangement.
    (b) A charge \(q_0\) is brought to the centre \(E\) of the square, the four charges being held fixed at its corners. How much extra work is needed to do this?
  
Solution:
    (a) Since the work done depends on the final arrangement, we calculate work needed for one way of adding the charges at \(A, B, C, D\):
    (i) Work needed to bring \(+q\) to \(A\): 0.
    (ii) Work to bring \(-q\) to \(B\) when \(+q\) at \(A\):
    \[
    -q \times \left(\frac{q}{4\pi\varepsilon_0 d}\right)
    = -\frac{q^2}{4\pi\varepsilon_0 d}
    \]
    (iii) Work to bring \(+q\) to \(C\) when \(+q\) at \(A\), \(-q\) at \(B\):
    \[
    +q \left( \frac{q}{4\pi\varepsilon_0 d\sqrt{2}} - \frac{q}{4\pi\varepsilon_0 d} \right)
    = -\frac{q^2}{4\pi\varepsilon_0 d}(1-\frac{1}{\sqrt{2}})
    \]
    (iv) Work to bring \(-q\) to \(D\) after other three charges:
    \[
    -q\left(\frac{q}{4\pi\varepsilon_0 d} - \frac{q}{4\pi\varepsilon_0 d\sqrt{2}} + \frac{q}{4\pi\varepsilon_0 d} \right)
    = -\frac{q^2}{4\pi\varepsilon_0 d}\left(2-\frac{1}{\sqrt{2}}\right)
    \]
    Add up all steps:
    \[
    = -\frac{q^2}{4\pi\varepsilon_0 d}\left[0 + 1-\frac{1}{\sqrt{2}} + 2-\frac{1}{\sqrt{2}}\right]
    = -\frac{q^2}{4\pi\varepsilon_0 d}\left(4-\sqrt{2}\right)
    \]
    (b) The extra work to bring a charge \(q_0\) to centre \(E\) when all corner charges are fixed is \(q_0 \times\) (potential at \(E\)), but potential there is zero due to symmetry, so the extra work required is zero.
  
Example 2.4
Four charges are arranged at the corners of a square ABCD of side d. (a) Find the work required to put together this arrangement. (b) Calculate extra work needed to bring a charge q₀ to the center.
Step 1: Bring +q to A
No work required (no other charges present)
W₁ = 0
Step 2: Bring -q to B
W₂ = -q × VB = -q²/(4πε₀d)
= -1.00 ×10⁻⁹ J
Step 3: Bring +q to C
W₃ = +q × (VC from A & B)
= -q²/(4πε₀d)(1-1/√2)
= -0.29 ×10⁻⁹ J
Step 4: Bring -q to D
W₄ = -q × (VD from A, B & C)
= -q²/(4πε₀d)(2-1/√2)
= -1.29 ×10⁻⁹ J
Total Work Required
Wtotal = W₁ + W₂ + W₃ + W₄ = -q²/(4πε₀d)(4-√2)
= -2.59 ×10⁻⁹ J
Key Observations
- The work done depends only on the final arrangement, not the assembly process
- This work equals the total electrostatic potential energy of the system
- Potential at center is zero (equal and opposite contributions cancel)
- No work is needed to bring a charge to the center



