Physics·Definition

Electric Field — Definition

NEET UG
Version 1Updated 22 Mar 2026

Definition

Imagine you have an electric charge, let's call it the 'source charge'. This source charge creates an invisible influence or 'field' around itself. This field is what we call the electric field. It's like a gravitational field around a planet – you can't see it, but you know it's there because if you put another object (like a satellite) into it, that object will experience a force.

Similarly, if you place another charge, called a 'test charge', into this electric field, it will experience an electric force.

The electric field at any point in space tells us two things: first, how strong the electric influence is at that point (its magnitude), and second, in which direction a positive test charge would be pushed or pulled if placed there (its direction).

Since it has both magnitude and direction, the electric field is a vector quantity. We define it precisely as the electric force per unit positive test charge. So, if a small positive test charge q0q_0 experiences a force F\vec{F} at a certain point, the electric field E\vec{E} at that point is simply E=Fq0\vec{E} = \frac{\vec{F}}{q_0}.

Why do we use a 'vanishingly small' positive test charge? Because we want to measure the field created *only* by the source charge, without the test charge itself significantly altering the original field.

If the test charge were large, its own field would interact with the source charge, changing the very field we are trying to measure. By making it infinitesimally small, we ensure it doesn't disturb the source charge's field.

The 'positive' convention is just that – a convention. It helps us consistently define the direction of the field: away from a positive source charge and towards a negative source charge. The unit for electric field is Newtons per Coulomb (N/C), which makes sense as it's force (Newtons) per charge (Coulomb).

Understanding the electric field is crucial because it allows us to analyze electrostatic interactions without always having to consider the specific 'test charge' experiencing the force; we can describe the 'state' of space itself due to the presence of charges.

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