Online Electrical Engineering
SI System of Units
Vector Algebra | Vector Diagram
Vector Diagram | Three Phase Vector Diagram
Nature of Electricity
Drift Velocity Drift Current and Electron Mobility
Electric Current and Theory of Electricity | Heating & Magnetic Effect
Voltage or Electric Potential Difference
Electrical Conductance Conductivity of Metal Semiconductor and Insulator | Band Theory
Electrical Resistance and Laws of Resistance
Types of resistor Carbon Composition and Wire Wound Resistor
Varistor Metal Oxide Varistor is nonlinear Resistor
Potentiometer Working Principle of Potentiometer
Variable Resistors | Defination, Uses and Types of Variable Resistors
Electric Power Single and Three Phase Power Active Reactive Apparent
Three Phase Circuit | Star and Delta System
Static Electric Field | Electrostatic Induction | Electric Field Strength
Magnetic Field and Magnetic Circuit | Magnetic Materials
Fleming Left Hand rule and Fleming Right Hand rule
What is Inductor and Inductance | Theory of Inductor
What is Capacitor and Capacitance? Types of Capacitors
Seebeck Effect and Seebeck Coefficient
Electric Lamp | Types of Electric Lamp
Cyclotron Basic Construction and Working Principle
Ionization Process and Definition
Principle of Electrolysis of Copper Sulfate Electrolyte
Applications of Electrolysis Electroplating Electroforming Electrorefining
Static Electric Field | Electrostatic Induction | Electric Field Strength
Under Basic Electrical Engineering
Definition of Electric FieldThe field surround an static electric charge is known as Static Electric Field. We know there are two types of charge present in the nature (i) positive and (ii) negative charge. In positive charge, there is mainly deficiency of electrons and in negative charge there are excess of electrons. Now, we can simply understand the concepts of charge from a very basic example. Take a dry comb, comb your hair (which should be dry) two to three times, now take that comb near tiny pieces of paper, you will see that the paper pieces are getting attracted to the comb. This is the very basic example of electric charge and static electric field. Due to friction there is movement of electrons between comb and hair, so one of them gets positively charged and another one gets negatively charged and as the paper is neutral (i.e. not charged) they get attracted to the comb. So, we can see that there is an attraction force works between charged particle and neutral particle, it has been seen further that there is repulsion between two same charged particles and attraction between two differently or opposite charged particles. This happens due to the field created around a particle. This can be understood if we imagine a glowing bulb, the bulb can be taken as the charge and the visible light can be compared to static electric field, the characteristic of field is similar to the light in the sense that the intensity of the field is greater near the source and it fades as we move further from the source. Now from another point of view we can say that static electric field is nothing but an intense space, in terms of power where work is done or needed to be done upon in presence of an electrically charged particle depending on the nature of the charged particle.
Electrostatic InductionA positive charge lacks electrons, where as a negative charge has excess electrons. What about the phenomenon of attraction of a neutral particle by a charged particle, because we can understand the phenomenon of attraction and repulsion between oppositely charged particles and same charged particles, but how neutrally charged particles get attracted by charged particles. This can be explained by electrostatic induction. The word induction itself explains a lot, it means action which is not the result of direct contact. To explain the above explained phenomenon, we can say that when a neutral body is brought near the charged body, due to influence of static electric field, free electrons inside the neutral body either come nearer to the charged body or go away from charged body depending upon the nature of charge in the charged body. If the charged body is positive, free electrons of the neutral body come nearer to the charged body and if the charged body is negative, the free electrons go away from the charged body. Thus, opposite charge is induced in the neutrally charged body near to the charged body and same charge on the opposite side. In this way, the portion of the neutral body nearer to the charged body is induced by opposite static charge and hence it would be attracted by charged body. We can understand the phenomenon more accurately by a diagram.
Electric Field Strength or Electric Field IntensityThe force acting on a unit positive charge inside an electric field is termed as electric field strength We discussed earlier, what is electric field. Now in this article we will know about electric field strength. Electric field strength can be determined by Coulomb’s law. According to this law, the force ‘F’ between two point charges leaving charge ‘Q1’ and Q2 and placed at a distance ‘d’ from each other is given by,
Where K is any constant, in SI system the force between two charges is given by
Here εo is the permittivity of vacuum = 8.854 x 10 − 12 F/m and εr is the relative permittivity of the surrounding medium. Now if Q2 = + 1 Coulomb, then
This equation shows the force acting the a unit positive charge placed at a distance d from charge Q1. As per definition this is nothing but of electric field strength of charge Q1 at a distance d from that charge. This field strength can also be written as,
Depending on this expression, the electric field strength can be expressed in Newton/Coulomb and it can also be expressed as Volt/Meter (volts per meter). [ This can be proved that these two unit are equivalent.] The electric field strength has direction and hence it is vector quantity.
Intensity means the magnitude or amount. Now field intensity similarly means the magnitude of the strength of the field. Finally electric field intensity or strength can be written as,
Video on Electric Field
Electric Field Due to a Point ChargeIf we consider a point charge of Q Coulomb, the total number of flux radiating from the charge (Q Coulombs) is equal to Q coulombs.
Electric Flux DensityThe tube forces which are termed as electric flux, radiate normally from the entire surface enclosing a point charge is nothing but the total charge of the point. Now, the amount of radiating this flux through unit surface area on the imaginary enclosure of the charge, is known as electric flux density. The unit of this is coulombs/m2.
Let's take a point charge of Q coulomb and place it at the center of a sphere of radius ’r’ then the electric flux density is
From the above relation we can see that the electric flux density does not depend on the medium, i.e. the absolute permittivity and relative permittivity, and it is inversely proportional with the square of the distance from the charge.
We know that electric field intensity or electric field strength is given as
Hence, the relation between electric field intensity and electric flux density is given by the equation
Electric Dipole MomentElectric dipole is created by two opposite and equal charges, a certain distance apart. It is equal to the product of one charge and the distance between them. Say two charges + Q and – Q apart from each other by a distance a. Then as per definition, electric dipole moment,
This is a vector quantity directed from negative to positive charge.
Electric dipole in Electric FieldWhen an electric dipole is placed inside a uniform electric field, the negative end of the dipole is attracted by positive end of the field and positive end of the dipole is attracted by negative end of the field. Due to these two forces, which are opposite in direction, there would be a torque acting on the dipole body. Let this torque is τ and θ is the angle between electric dipole and electric field. The amplitude of force acting on charge Q in the electric field E is given as EQ.
Due to this field the dipole will be oriented parallel to the electric field. Now let us calculate how much work to be done for this parallel orientation of dipole along the field. If due to this electric dipole moment, the orientation of dipole changes from θ1 to θ2. So work done for this angular moment is given as,
This is the work done by electric field which will be stored as potential energy in the dipole. If dipole is aligned from its vertical position to parallel position with respect to direction of electric field. The Work done or potential energy stored is