The electric field of a signed point electric charge in vacuum follows Coulomb's law:
For the conducting plane, the method of images replaces each charge at height by an image charge at height . The real and image electric fields have cancelling tangential components and equal normal components at the surface. Thus the electric field at a conducting plane from axial point charges, just above the point directly below them, is
Numerically,
The surface value means the air-side limit. Inside the ideal conductor the electrostatic electric field is zero; its discontinuity across the surface is supported by induced surface charge. Omitting the image charges would give half the external answer.

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