Electrical and Electronics Engineering Books
Basic Construction of Wind TurbineClosely Related Articles
Electrical Conductance Conductivity of Metal Semiconductor and Insulator | Band Theory
Properties of Electric Conductor
Electrical Resistance and Laws of Resistance
What is Capacitor and Capacitance? Types of Capacitors
Working Principle of a Capacitor
Energy Stored in Capacitor
Quality Factor of Inductor and Capacitor
Transient Behavior of Capacitor
Capacitors in Series and Parallel
Testing of Capacitor Bank
How to Test Capacitors?
Electric Circuit and Electrical Circuit Elements
Series Parallel Battery Cells
Electrical DC Series and Parallel Circuit
RL Series Circuit
Three Phase Circuit | Star and Delta System
RL Parallel Circuit
RL Circuit Transfer Function Time Constant RL Circuit as Filter
Construction of AC Circuits and Working of AC Circuits
Series RLC Circuit
Parallel RLC Circuit
Resistances in Series and Resistances in Parallel
Resonance in Series RLC Circuit
Planar and Non Planar Graphs of Circuit
Earn with us
Electric Current and Theory of Electricity | Heating and Magnetic Effect
Nature of Electricity
Drift Velocity Drift Current and Electron Mobility
Electric Current and Voltage Division Rule
RMS or Root Mean Square Value of AC Signal
What is Electric Field?
Electric Field Strength or Electric Field Intensity
Static Electric Field | Electrostatic Induction
What is Flux? Types of Flux?
Magnetic Field and Magnetic Circuit | Magnetic Materials
Energy Stored in a Magnetic Field
A Current Carrying Conductor Within A Magnetic Field
Hard Magnetic Materials
Soft Magnetic Materials
Magnetic Circuit with Air Gap
Fourier Series and Fourier Transform
Trigonometric Fourier Series
Analysis of Exponential Fourier Series
Electrical and Electronics Engineering Books
What is Inductor and Inductance | Theory of Inductor
SI System of Units
Electrical International Symbol
Electric Power Single and Three Phase Power Active Reactive Apparent
Vector Algebra | Vector Diagram
Relationship of Line and Phase Voltages and Currents in a Star Connected System
Vector Diagram | Three Phase Vector Diagram
Types of resistor Carbon Composition and Wire Wound Resistor
Varistor Metal Oxide Varistor is nonlinear Resistor
Carbon Composition Resistor
Wire Wound Resistor
Variable Resistors | Defination, Uses and Types of Variable Resistors
Light Dependent Resistor | LDR and Working Principle of LDR
Source of Electrical Energy
Ideal Dependent Independent Voltage Current Source
Voltage or Electric Potential Difference
Voltage in Series
Voltage in Parallel
Voltage Drop Calculation
Voltage Regulator 7805
Voltage to Current Converter
Electrical Resistance and Laws of Resistance
Definition of ResistanceElectrical resistance may be defined as the basic property of any substance due to which it opposes the flow of current through it. While a voltage is applied across any substance, current starts flowing through it. But if we observe carefully, the current flows through the all substances are not equal even when the same voltage is applied across each of the substances. This is because current carrying capacity of all substances is not equal. The current depends upon the number of electrons' crosses the cross-section per unit time. Again this number of electrons crossing the cross-section is dependable on the free electrons available in the substances. If free electrons are plenty in a substance, the amount of current is more for same applied voltage across the substances.
The current through a substance not only depends upon the number of free electrons in it, but also depends upon the length of path an electron has to travel to reach from lower potential end to higher potential end of the substance. In addition to that, every electron has to collide randomly with other atoms and electrons in numbers of times during its traveling. So, every substance has a property to resist current through it and this property is known as electric resistance. If one volt across a conductor produces one ampere of current through it, then the resistance of the conductor is said to be one ohm (Ω).
Laws of ResistanceThere are mainly two laws of resistance from which the resistivity or specific resistance of any substance can easily be determined. One law is related to cross-sectional area of the conductor and other law is related with its length.
If the length of the conductor is increased, the path traveled by the electrons is also increased. If electrons travel long, they collide more and consequently the number of electron passing through the conductor becomes less; hence current through the conductor is reduced. In other word, resistance of the conductor increases with increase in length of the conductor. The laws of resistance state that, Electrical resistance R of a conductor or wire is
- directly proportional to its length, l i.e. R ∝ l,
- inversely proportional to its area of cross-section, a i.e.
Unit of ResistivityThe unit of resistivity can be easily determined form its equation The unit of resistivity is Ω-m in MKS system and Ω-cm in CGS system and 1 Ω-m = 100 Ω-cm.
Temperature Coefficient of Resistance and Inferred Zero Resistance Temperature
|Materials||Resistivity in μ Ω-cm at 20oC||Temperature Coefficient of Resistance in Ω per oC at 20oC||Inferred Zerro Resistance Temperature in oC|
|Brass||6 to 8||0.0020||- 480|
|Carbon||3k to 7k||0.00005|
|Manganin||42 to 74||0.00003||- 236|
Resistance Variation with TemperatureThere are some materials mainly metals, such as silver, copper, aluminum, which have plenty of free electrons. Hence this type of materials can conduct current easily that means they are least resistive. But the resistivity of these materials is highly dependable upon their temperature. Generally metals offer more electrical resistance if temperature is increased. On the other hand the resistance offered by a non - metallic substance normally decreases with increase of temperature. If we take a piece of pure metal and make its temperature 0° by means of ice and then increase its temperature from gradually from 0°C to to 100°C by heating it. During increasing of temperature if we take its resistance at a regular interval, we will find that electrical resistance of the metal piece is gradually increased with increase in temperature. If we plot the resistance variation with temperature i.e. resistance Vs temperature graph, we will get a straight line as shown in the figure below. If this straight line is extended behind the resistance axis, it will cut the temperature axis at some temperature, - t0°C. From the graph it is clear that, at this temperature the electrical resistance of the metal becomes zero. This temperature is referred as inferred zero resistance temperature. Although zero resistance of any substance cannot be possible practically. Actually rate of resistance variation with temperature is not constant throughout all range of temperature. Actual graph is also shown in the figure below. Let's R1 and R2 are the measured resistances at temperature t1°C and t2°C respectively. Then we can write the equation below, From the above equation we can calculate resistance of any material at different temperature. Suppose we have measured resistance of a metal at t1oC and this is R1. If we know the inferred zero resistance temperature i.e. t0 of that particular metal, then we can easily calculate any unknown resistance R2 at any temperature t2°C from the above equation.
The resistance variation with temperature is often used for determining temperature variation of any electrical machine. For example, in temperature rise test of transformer, for determining winding temperature rise, the above equation is applied. This is impossible to access winding inside the an electrical power transformer insulation system for measurement of temperature but we are lucky enough that we have resistance variation with temperature graph in our hand. After measuring electrical resistance of the winding both at the beginning and end of the test run of the transformer, we can easily determine the temperature rise in the transformer winding during test run. 20°C is adopted as standard reference temperature for mentioning resistance. That means if we say resistance of any substance is 20 Ω that means this resistance is measured at the temperature of 20°C.
Video Resistance Variation with Temperature
resistance variation with temperaturethat electrical resistance of every substance changes with change in its temperature. Temperature coefficient of resistance is the measure of change in electrical resistance of any substance per degree of temperature rise. Let a conductor having a resistance of R0 at 0°C and Rt at t°C respectively. From the equation of resistance variation with temperature we get This αo is called temperature coefficient of resistance of that substance at 0°C. From the above equation, it is clear that the change in electrical resistance of any substance due to temperature rise mainly depends upon three factors-
- The value of resistance at initial temperature,
- Rise of temperature and
- the αo.
So the temperature coefficient of resistance at 0°C of any substance is the reciprocal of the inferred zero resistance temperature of that substance.
So far we have discussed about the materials that resistance increases with increase in temperature, but there are many materials that's electrical resistance decreases with decrease in temperature. Actually in metal if temperature is increased, the random motion of charged particles inside the materials increases which results to more collisions. More collision resist smooth flow of electrons through the metal, hence the resistance of the metal increases with the increase in temperature. So, temperature coefficient of resistance is considered as positive for metal. But in case of semiconductor or other non - metal, the number of free electrons increases with increase in temperature. That means if temperature increases, more number of electrons comes to the conduction bands from valance band by crossing the forbidden energy gap. As the number of free electrons increases, the resistance of this type of non-metallic substance decreases with increase of temperature. Hence temperature coefficient of resistance is negative for non-metallic substances and semiconductors. If there is approximately no change in resistance with temperature, the value of this coefficient is considered as zero. Such as alloys like constantan and manganin that's temperature coefficient of resistance is nearly zero. The value of this coefficient is not constant, it depends upon the initial temperature on which the increment of resistance is based. When the increment is based on initial temperature of 0°C, the value of this coefficient is αo - which is nothing but the reciprocal of the respective inferred zero resistance temperature of the substance. But at any other temperature, temperature coefficient of electrical resistance is not same as this αo. Actually for any material, the value of this coefficient is maximum at 0°C temperature. Say the value of this coefficient of any material at any t°C is αt, then its value can be determined by the following equation, The value of this coefficient at a temperature of t2°C in the term of the same at t1°C is given as,