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Nature of Electricity
Drift Velocity Drift Current and Electron Mobility
Electric Current and Theory of Electricity | Heating & Magnetic Effect
Voltage or Electric Potential Difference
Atomic Structure
Electrical Conductance Conductivity of Metal Semiconductor and Insulator | Band Theory
Electrical Resistance and Laws of Resistance
SI System of Units
Ideal Dependent Independent Voltage Current Source
Series Parallel Battery Cells
Single and Multi Mesh Analysis
Kirchhoff Current Law and Kirchhoff Voltage Law
Superposition Theorem
Reciprocity Theorem
Compensation Theorem
Electric Power Single and Three Phase Power Active Reactive Apparent
Types of resistor Carbon Composition and Wire Wound Resistor
Varistor Metal Oxide Varistor is nonlinear Resistor
Principle of Electrolysis of Copper Sulfate Electrolyte
Construction of Lead Acid Battery
Voltaic Cell
Norton Theorem | Norton Equivalent Current and Resistance
Maximum Power Transfer Theorem
Working of Lead Acid Battery | Lead Acid Secondary Storage Battery
Fleming Left Hand rule and Fleming Right Hand rule
Ohms Law | Equation Formula and Limitation of Ohms Law
Electrical DC Series and Parallel Circuit
Ionization Process and Definition
Faraday First and Second Laws of Electrolysis
Applications of Electrolysis Electroplating Electroforming Electrorefining
Resistances in Series and Resistances in Parallel
Delta - Star transformation | Star - Delta Transformation
Tellegen Theorem
Thevenin Theorem and Thevenin Equivalent Voltage and Resistance
Vector Algebra | Vector Diagram
Wheatstone Bridge Circuit Theory and Principle
Vector Diagram | Three Phase Vector Diagram
Static Electric Field | Electrostatic Induction | Electric Field Strength
Joules Law of Heating
Gauss Theorem
Alkaline Batteries
Nickel Iron Batteries or Edison Batteries
Three Phase Circuit | Star and Delta System
Potentiometer Working Principle of Potentiometer
Lenz Law of Electromagnetic Induction
Seebeck Effect and Seebeck Coefficient
Faraday Law of Electromagnetic Induction
RL Series Circuit
RLC Circuit
RL Circuit Transfer Function Time Constant RL Circuit as Filter
Battery | History and Working Principle of Batteries
RL Parallel Circuit
Series RLC Circuit
Coulombs Law | Explanation Statement Formulas Principle Limitation of Coulomb’s Law
Voltage Divider
Resonance in Series RLC Circuit
Parallel RLC Circuit
Aluminum Air Battery | Experiment Reaction Equations Uses
Kelvin Bridge Circuit | Kelvin Double Bridge
Magnetic Field and Magnetic Circuit | Magnetic Materials
Biot Savart Law
What is Capacitor and Capacitance? Types of Capacitors
Zinc Carbon Battery |Types of Zinc Carbon Battery | Advantages and Disadvantages
Mercuric Oxide Battery | Chemistry Construction Advantages Uses
Variable Resistors | Defination, Uses and Types of Variable Resistors
Electric Lamp | Types of Electric Lamp
What is Inductor and Inductance | Theory of Inductor
Charging of Battery and Discharging of Battery
Magnesium Battery | Chemistry Construction of Magnesium Battery

Static Electric Field | Electrostatic Induction | Electric Field Strength

Under Basic Electrical Engineering

Definition of Electric Field

The 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 Induction

A 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. electrostatic induction

Electric Field Strength or Electric Field Intensity

The 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

We know that there is an electric field around a charge, and whenever there is an electric field there is electric flux around it, this field though theoretically assumed to be spread up to infinity but practically they are taken to be composed of small closed space. Now from each point of charged surface, electric field tube force emerges, which radiates through the surrounding. This total number of force tube is called electric flux. The field is nothing but an energy field, i.e. to go through the field work is done by or done upon a point charge. So, there must be some kind of energy present in the electric field.

Electric Field Due to a Point Charge

If 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 field due to point charge

Electric Flux Density

The 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 Moment

Electric 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 Field

electric dipole moment When 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

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