Step 1: Understanding the Concept
Both charges are of the same sign, so their fields cancel at a point between them.
Step 2: Equation
At distance \(x\) from \(8q\): \(\dfrac{k\,8q}{x^2}=\dfrac{k\,2q}{(L-x)^2}\), so \(\dfrac{4}{x^2}=\dfrac{1}{(L-x)^2}\).
Step 3: Calculation
Taking the square root, \(\dfrac{2}{x}=\dfrac{1}{L-x}\), so \(2L-2x=x\).
Step 4: Result
\(x=\dfrac{2L}{3}\), which lies between 0 and \(L\).
Final Answer:
The field is zero at x equal to 2L/3 from the origin.
\[ \boxed{\text{(A) }\dfrac{2L}{3}} \]