Lectures on Electricity and Magnetism — new series of lectures – EML – 1

All articles in this series will be found here. Click on link to left or search for menu “E AND M BASICS” on top.

## Electric Field and Gauss Law

## Electric Field

Electric field is the amount of Coulomb’s force, that a positive charge of 1 unit experiences at a given position. Its a vector in the same direction as that of the electric force. We will discuss the time independent electric field which is also known as the static field.

### Advantage of electric field

**Advantage over electric force**: Coulomb’s force law is a non-local expression, its a action-at-a-distance type quantity, i.e. the force is here at this instant and at any arbitrary distance apart at the same instant, it doesn’t get relayed, its instantaneous. This force which is supposed to transmit at infinite speed thus violates the special theory of relativity, where all speeds are bound by the limit of speed of light in free space. According to the postulate of this theory information can’t transmit faster than speed of light in vacuum. But field formulation is local, its compatible with special theory of relativity.**Electric fields are vector fields**: there is a vector associated with every point in space and time. Once the field is known we don’t worry about nature of sources that produce these field. Physics becomes simpler as a consequence.

**+ click to see more about this article**

This article belongs to a group of lectures I intend to prepare for their online dissemination — these were delivered in a physical format, beginning with hand written notes that were delivered in a classroom full of students. This series is on Electricity and Magnetism and bears the name sake *Electricity and Magnetism Lectures* and the number of the lecture will be appended to the end to reflect the same. eg the current lecture will be named EML – 1 . This lecture was delivered to honors students on 30th Jan 2017.

In the meanwhile if you can’t wait and you need some of these concepts at the earliest, here is a slide-share presentation I had made roughly 5 years ago that consists of “some of the things” an undergrad needs: *Electricity and Magnetism* slides. There are other slides on different topics at that account of mine on **slideshare.net** (such as; Introduction to Quantum Mechanics , and these are quite well received by the community for their usefulness).

### Electric field lines or lines of force

Since electric field is a vector field (you can see much detail regarding vector fields here) there is a vector associated with every point in space (in static situation we disregard time). Therefore we can draw the direction of the vector at each point in space. If direction vectors are drawn at close points we obtain continuous curves. The tangent to these curves represent direction of electric field at these points and the lines drawn with direction are known as “**electric field lines** or **electric lines of force**“.

Electric field lines and lines of force are synonymous, they are one and the same, but thats not true for magnetic field lines, they are always different from magnetic lines of force.

This is due to definition of magnetic field from Lorentz force which is a cross product of two vectors.

The following diagrams represent the lines of force for electric field created by a single positive charge, a single negative charge and an electric dipole.

#### Nature of electric lines of force

- The electric field due to point charges are very large (in magnitude) and are radially outward for +ve charges or radially inward for -ve charges. See diagrams above. Other charges can not produce such patterns of lines of force. So presence of such patterns of radial lines of force is a signature of point charges.
- Electric lines of force tells us the direction of electric field at any point.
- Density of electric field lines gives the relative magnitude of electric field (strength). High density means large electric field strength.

### Electric flux

If electric field ** E** is present in a region of infinitesimal area element

**then the electric flux is defined as . Here the unit vector**

*dA***is defined as the normal to the surface area**

*n**dA*. For closed surface we are not free to define whether the surface has a positive or negative

**. For example for a spherical surface**

*n***is always outward.**

*n*For a large surface (i.e. one which isn’t uniform like an infinitesimal one) we need to integrate over all elements of the surface to find the flux.

The total outward flux across a closed surface due to charges present outside of it is zero. This is because as much flux enters the surface, as exits.

Flux would accumulate inside of a closed surface only if net charge accumulates.

### Gauss Law

Consider a +ve point charge *q* at the center of a spherical surface S of radius *R*.

The electric field ** E** due to the charge

*q*is given by Coulomb’s law: . The area of the sphere is

*4πR*. The field

^{2}**and the outward normal to the surface S are along the same direction: this gives dot product between**

*E***and normal vector**

*E***= magnitude of**

*n***. Thus total outward flux is given by: . But this result is valid for surface of any shape.**

*E*Lets consider two surfaces S and S’ as shown in the following diagram, S’ has an arbitrary shape, S is spherical. The flux due to *q* at the surface of S is *-Φ = – 4πkq*, since outward normal to S is towards *q*. But for the region inside S’ and S there is no charge. We just learned that if there is no charge enclosed in a surface then total flux is zero, So, outward flux of S’ must be *+Φ*.

So Gauss law can be stated in the following form; total outward electric flux across any closed surface enclosing a charge *Q* is *Φ = 4πkQ*. Gauss law can be used with symmetry to evaluate unknown electric fields in many situations.

#### Illustration of Gauss Law with spherical symmetry

Calculate the electric field due to an uniformly charged sphere of radius *R* carrying a charge *Q* at a point P situated at a distance *r > R*, from its center.

Due to spherical symmetry the field at point P is unchanged if we rotate the sphere about the radial line. Lets denote this field as *E(r)* since it depends only on radial position *r* and not the azimuthal angle coordinate φ or polar angle wrt zenith coordinate *θ*.

*Φ = E(r) × area of the spherical surface = 4πr ^{2}E(r)*, but flux is given by Gauss law as;

*flux = Φ = 4πkQ*. So

*. Thus the field is given as*

*4πr*=^{2}E(r)*4πkQ**E(r) = kQ/*. This is same as the field that would be produced at that point P, by a point charge, located at the center of the sphere.

*r*^{2}
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