
Gauss's Law, also known as Gauss's flux theorem, is a law relating the distribution of electric charge to the resulting electric field. The law was formulated by Carl Friedrich Gauss in 1835 but was not published until 1867. Electric flux is the rate of flow of the electric field through a given area. Gauss's Law describes the electric flux over a surface as the surface integral. The net outward normal electric flux through any closed surface is proportional to the total electric charge enclosed within that closed surface. The sense or direction of the net electric flux (inward or outward) depends on the sign of the enclosed charge. Charges outside the enclosed volume do not produce a net electric flux through the surfaces.
| Characteristics | Values |
|---|---|
| Definition | Gauss's law is a law relating the distribution of electric charge to the resulting electric field. |
| Formula | \(\Phi_E\equiv\int \vec{E}\cdot d\vec{A}=\frac{Q_\text{enclosed}}{\epsilon_o}\) |
| Relation to Permittivity | Flux is inversely proportional to permittivity. |
| Relation to Electric Flux | Electric flux is the rate of flow of the electric field through a given area. |
| Relation to Coulomb's Law | Gauss's law can be used to derive Coulomb's law, and vice versa. |
| Applicability | Gauss's law holds for all situations but is only useful for "by hand" calculations when high degrees of symmetry exist in the electric field. |
| Units | Electric flux has SI units of volt meters (V m), or newton meters squared per coulomb (N m2 C-1). |
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What You'll Learn

Electric flux defined
Electric flux is a property of an electric field that can be thought of as the number of electric lines of force (or electric field lines) that intersect a given area. Electric field lines originate on positive electric charges and terminate on negative charges. The total number of electric field lines passing through a given area in a unit of time is defined as the electric flux.
The electric flux through a surface is given by the surface integral: ΦE = ∫∫_S E . dA. Here, E is the electric field and dA is an infinitesimal area on the surface with an outward-facing surface normal defining its direction. The SI unit of electric flux is the volt-meter (V·m), or newton-metre squared per coulomb (N·m2·C−1). Thus, the SI base units of electric flux are kg·m3·s−3·A−1.
For a non-uniform electric field, the electric flux (dΦE) through a small surface area (dA) is given by the equation dΦE = E . dA. This is the electric field (E) multiplied by the component of the area (dA) perpendicular to the field. The direction of the net electric flux (inward or outward) depends on the sign of the enclosed charge. Charges outside the enclosed volume do not produce a net electric flux through the surfaces.
A Gaussian surface is an arbitrary closed surface in three-dimensional space through which the flux is calculated. It is used in conjunction with Gauss's law for the corresponding field by performing a surface integral to calculate the total amount of the source quantity enclosed.
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Gauss's Law explained
Gauss's Law, also known as Gauss's flux theorem, is a law that relates the distribution of electric charge to the resulting electric field. The law was formulated by Carl Friedrich Gauss in 1835 but was not published until 1867. It is one of the four Maxwell's equations that form the basis of classical electrodynamics.
Gauss's Law can be used to derive Coulomb's law, and vice versa. It is important to note that while Coulomb's law only applies to stationary charges, Gauss's law holds for moving charges as well, making it more general. Gauss's law states that the net outward normal electric flux through any closed surface is proportional to the total electric charge enclosed within that closed surface. In simpler terms, the law states that the total electric flux through any closed surface is proportional to the total (net) electric charge inside the surface.
Electric flux refers to the rate of flow of the electric field through a given area. It is the amount of electric field penetrating a surface, which can be open or closed. For a non-uniform electric field, the electric flux through a small surface area is given by the electric field, E, multiplied by the component of the area perpendicular to the field. Gauss's Law describes the electric flux over a surface as the surface integral, where E is the electric field and dS is a differential area on the closed surface with an outward-facing surface normal defining its direction.
Gaussian surfaces are chosen to simplify the calculation of the surface integral. The Gaussian surface is selected such that for every point on the surface, the component of the electric field along the normal vector is constant, allowing for easier integration. The choice of a spherical Gaussian surface, for example, can be made to exploit the symmetry of the configuration.
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The relationship between electric flux and Gauss's Law
Gauss's law, or Gauss's flux theorem, is a law that relates the distribution of electric charge to the resulting electric field. It states that the net outward normal electric flux through any closed surface is directly proportional to the total electric charge enclosed within that closed surface. This is independent of the size of the closed surface.
Mathematically, Gauss's law can be expressed using vector calculus in integral form and differential form, with both being equivalent since they are related by the divergence theorem, also known as Gauss's theorem. The integral form of Gauss's law is given as:
> ΦE = ∫∫ E . dA
Where ΦE is the electric flux, E is the electric field, and dA is the vector area.
The differential form of Gauss's law relates the electric field to the charge distribution at a particular point in space. According to the law, the divergence of the electric field (E) will be equal to the volume charge density (ρ) at a particular point.
Gauss's law is particularly useful for "by hand" calculations when high degrees of symmetry exist in the electric field, such as spherical and cylindrical symmetry. It is used to determine the electric field of charge distributions with symmetry.
> Φ = E * S * cos(θ)
Where Φ is the electric flux, E is the magnitude of the electric field, S is the area of the surface, and θ is the angle between the electric field lines and the normal (perpendicular) to S.
In summary, Gauss's law describes the relationship between electric flux and the total electric charge enclosed within a closed surface, providing a framework for understanding the distribution of electric charge and the resulting electric field. Electric flux, on the other hand, represents the flow of electric field lines through a surface and is influenced by factors such as the electric field, area, and angle between them.
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The role of permittivity in Gauss's Law
Gauss's Law, formulated by Carl Friedrich Gauss in 1835, relates the distribution of electric charge to the resulting electric field. It states that the net outward normal electric flux through any closed surface is proportional to the total electric charge enclosed within that closed surface.
Electric flux is the rate of flow of the electric field through a given area. The role of permittivity in Gauss's Law is crucial in understanding the behaviour of electric fields in different media. Permittivity is a property of a material that describes how easily electric fields can be established within it. It is a measure of how well a material can polarize in response to an applied electric field.
In the context of Gauss's Law, permittivity is represented by the symbol ε0 and is also known as the vacuum permittivity or the permittivity of free space. It is a constant value that represents the ability of a vacuum to permit the establishment of an electric field. The permittivity of free space is used as a reference point to compare the permittivity of other materials.
When dealing with a closed surface enclosing no charge, the permittivity of the medium becomes important. In such cases, the electric field lines caused by charges outside the region do not produce a net flux within the closed surface. However, the permittivity of the medium can influence how these field lines interact with the enclosed space.
The permittivity of a material affects the strength of the electric field that can be established for a given charge. In other words, it determines how easily electric flux lines can pass through a material. Materials with higher permittivity allow for greater electric polarization and can accommodate more electric flux lines per unit area.
In summary, permittivity plays a fundamental role in Gauss's Law by quantifying the ability of a material to permit the establishment of an electric field. It influences the behaviour of electric flux lines and the overall strength of the electric field within a given medium. Understanding permittivity is crucial for applying Gauss's Law in practical calculations involving electric fields and charges in different materials.
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Applications of Gauss's Law
Gauss's law for electric fields is a powerful tool with a wide range of applications in physics, particularly in understanding electric flux and charge distribution. One of its key applications is in determining the relationship between electric flux and the total electric charge enclosed by a surface. Gauss's law states that the net electric flux passing through a closed surface is directly proportional to the total electric charge contained within that surface. This relationship holds regardless of the shape or size of the closed surface, making it a versatile principle.
The law also finds application in scenarios involving conductors set at known potentials. In such cases, Gauss's law enables us to determine the distribution of electric charge within a given region of the conductor. By integrating the electric field and considering its behaviour relative to the conductor's surface, we can deduce the charge distribution. This application is particularly valuable in understanding the behaviour of electric fields within conductors.
Gauss's law is closely related to Coulomb's law, and the two can be derived from each other. This mathematical similarity allows for a deeper understanding of the relationship between electric fields and charges. By considering the symmetry of the electric field and performing the necessary integrations, we can establish the connection between these two fundamental laws in physics.
Additionally, Gauss's law is applied in scenarios involving infinite wires or cylindrical symmetry. By considering the angles between the electric field and the area vector, we can determine the contribution of different surfaces to the overall electric flux. This application demonstrates how Gauss's law helps analyse complex charge distributions and their resulting electric fields.
The differential form of Gauss's law is also valuable in relating the electric field to the charge distribution at a specific point in space. According to the law, the divergence of the electric field (E) is equal to the volume charge density (ρ) at a given point. This application allows for a detailed analysis of how electric fields vary with changes in charge distribution, providing insights into the behaviour of electric fields in various scenarios.
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Frequently asked questions
Gauss's Law, also known as Gauss's flux theorem, relates the distribution of electric charge to the resulting electric field.
Electric flux is the rate of flow of the electric field through a given area. It is the amount of electric field penetrating a surface, which can be open or closed.
Gauss's Law states that the total electric flux through a closed surface is proportional to the total charge inside the surface. If there is no charge inside, the electric flux through the surface is zero.
The electric flux through a planar area is defined as the electric field times the component of the area perpendicular to the field. For a non-uniform electric field, the electric flux through a small surface area is given by the electric field, E, multiplied by the component of the area perpendicular to the field.
A Gaussian surface is an arbitrary closed surface in three-dimensional space through which the flux is calculated. It is chosen to exploit symmetries of a configuration, simplifying the calculation of the surface integral.











































