Setting up. The total field is the vector sum (superposition principle) of the three contributions Ei=ri2k∣qi∣. On an axis it is enough to manage the signs: take the +x direction as positive. The field of a positive charge points away from it, that of a negative charge points towards it. Using k=9⋅109.
Point A (x=0,25 m). Distances: r1=0,25, r2=0,25, r3=0,75.
E1E2E3=0,252(9⋅109)(2⋅10−6)=+2,88⋅105 (from q1+, towards +x)=0,252(9⋅109)(3⋅10−6)=+4,32⋅105 (towards q2− on the right, +x)=0,752(9⋅109)(5⋅10−6)=−0,80⋅105 (from q3+, towards −x)
EA=(2,88+4,32−0,80)⋅105⟹EA≈6,4⋅105 N/C (towards +x)
Point B (x=0,75 m). Distances: r1=0,75, r2=0,25, r3=0,25.
E1E2E3=0,752(9⋅109)(2⋅10−6)=+0,32⋅105 (from q1+, towards +x)=0,252(9⋅109)(3⋅10−6)=−4,32⋅105 (towards q2− on the left, −x)=0,252(9⋅109)(5⋅10−6)=−7,20⋅105 (from q3+, towards −x)
At B both q2 (attracting to the left) and q3 (repelling to the left) point in the same direction −x, so they add up:
EB=(0,32−4,32−7,20)⋅105⟹EB≈−1,1⋅106 N/C (towards −x)
Comparison. ∣EB∣≈1,1⋅106>∣EA∣≈6,4⋅105: the field is larger at B, because there the contributions of the negative charge q2 and the large positive charge q3 (both close, at 0,25 m) agree in direction, whereas at A they partly cancel.