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  1. Home
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  4. /Electric Field Calculator

Electric Field Calculator

Last updated: March 17, 2026

Calculator

Results

Electric Field Magnitude

898,755.17923

N/C

Signed Field Value

898,755.17923

N/C

Electric Potential

89,875.517923

V

Force on Test Charge

0.089876

N

Force Magnitude on Test Charge

0.089876

N

Results

Electric Field Magnitude

898,755.17923

N/C

Signed Field Value

898,755.17923

N/C

Electric Potential

89,875.517923

V

Force on Test Charge

0.089876

N

Force Magnitude on Test Charge

0.089876

N

The Electric Field Calculator determines the electric field magnitude and direction produced by a point charge at a specified distance. The electric field is a fundamental concept in electrostatics, representing the force per unit charge that would be experienced by a small positive test charge placed at that point. Introduced by Michael Faraday, the electric field concept allows us to describe how charges influence the space around them without requiring a second charge to be present. The electric field due to a point charge follows an inverse-square law: $$E = k\frac{|q|}{r^2}$$, where k is Coulomb's constant. Electric fields are vector quantities — they point radially outward from positive charges and radially inward toward negative charges. This calculator also computes the force that the field exerts on an optional test charge (F = qE) and the electric potential at that location, providing a complete electrostatic picture of the point in space.

Visual Analysis

How It Works

The calculator uses the following equations from electrostatics:

$$E = k\frac{|q|}{r^2} = \frac{|q|}{4\pi\varepsilon_0 r^2}$$

where:

  • E is the electric field magnitude in N/C (or equivalently V/m)
  • k = 8.9875 × 10⁹ N·m²/C² is Coulomb's constant
  • q is the source charge in coulombs
  • r is the distance from the source charge in meters

The force on a test charge q₀ placed in this field is:

$$F = q_0 E$$

The electric potential at distance r from a point charge is:

$$V = k\frac{q}{r}$$

Unlike the electric field (a vector), the potential is a scalar quantity. The electric field points in the direction of decreasing potential, related by $$E = -\frac{dV}{dr}$$ for radial symmetry. The field direction is determined by the sign of the source charge: positive charges create fields pointing outward, while negative charges create fields pointing inward.

Understanding Your Results

The electric field magnitude tells you how strongly a charge influences the surrounding space at the given distance. The units N/C and V/m are equivalent. A field of 1000 N/C means a 1 C test charge would experience a force of 1000 N. The field direction indicates whether a positive test charge would be pushed away (positive source) or pulled toward (negative source) the source charge. The electric potential gives the work per unit charge needed to bring a test charge from infinity to that point. The force on the test charge shows the actual mechanical effect of the field on the specified test charge.

Worked Examples

Example 1: Field from a Microcoulomb Charge

Inputs

q0.000001
r0.1
test charge1e-7

Results

electric field899750
field directionRadially outward (away from +q)
force on test0.089975
potential89975

A +1 μC charge creates an electric field of approximately 899,750 N/C at a distance of 10 cm. The field points radially outward from the positive charge. A 0.1 μC test charge placed there would experience a force of about 0.09 N.

Example 2: Field from a Negative Charge

Inputs

q-0.000005
r0.2
test charge0.000001

Results

electric field1124688
field directionRadially inward (toward -q)
force on test1.124688
potential-224938

A −5 μC charge produces a field of about 1,124,688 N/C at 20 cm distance. The field points radially inward toward the negative charge. The negative electric potential indicates that positive charges are attracted toward this point.

Frequently Asked Questions

The electric field E at a point in space is the force per unit positive charge that would be experienced by a small test charge placed at that point: E = F/q₀. It is a vector field — it has both magnitude and direction at every point in space. The SI unit is newtons per coulomb (N/C) or equivalently volts per meter (V/m).

The electric field is a vector quantity representing force per unit charge (N/C), while the electric potential is a scalar quantity representing energy per unit charge (V = J/C). They are related: the electric field points in the direction of decreasing potential, and E = −dV/dr for radial fields. The potential is often easier to compute because scalar addition is simpler than vector addition.

Use the principle of superposition: the total electric field at any point is the vector sum of the fields due to each individual charge. Calculate each field separately using E = kq/r², then add them as vectors, accounting for their directions. For continuous charge distributions, replace the sum with an integral over the charge distribution.

Electric field lines are visual representations of the electric field. They start on positive charges and end on negative charges (or extend to infinity). The density of field lines is proportional to the field strength, and the tangent to a field line at any point gives the field direction. Field lines never cross, because the field has a unique direction at each point.

The inverse-square dependence arises from the geometry of three-dimensional space. The field from a point charge spreads uniformly over a spherical surface of area 4πr². As the radius doubles, the same total flux passes through four times the area, so the field intensity drops by a factor of four. This is a consequence of Gauss's Law and the 1/r² behavior is common to all central force fields in 3D space.

The Earth's fair-weather atmospheric electric field is about 100 V/m pointing downward. Near a Van de Graaff generator, fields reach 10⁶ V/m. The dielectric breakdown of air occurs at approximately 3 × 10⁶ V/m, producing sparks or lightning. Inside atoms, fields at the electron orbit reach about 5 × 10¹¹ V/m, demonstrating the enormous strength of electromagnetic forces at the atomic scale.

Sources & Methodology

Griffiths, D. J. (2017). Introduction to Electrodynamics (4th ed.). Cambridge University Press. Purcell, E. M., & Morin, D. J. (2013). Electricity and Magnetism (3rd ed.). Cambridge University Press. Young, H. D., & Freedman, R. A. (2019). University Physics (15th ed.). Pearson.
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