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Home » GATE Study Material » Electrical Engineering » Electrical Elements » Resistor

Resistor

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Resistor

Electrical engineers communicate with symbols. Circuit diagrams are abstract representations of real circuits and are composed of symbols for the various elements in the circuit. Here is the circuit symbol for a resistor.

The symbol for a resistor should include definitions for the voltage across the resistor and the current through the resistor. The definitions include:

  • A symbolic name for the variable ( Vr for the voltage and Ir for the current for the symbol shown above).
  • A definition of the polarity (Shown by "+" and "-" for the voltage and an arrow for the current).
Ohm's Law gives us a relationship between the voltage across a piece of conducting material (a resistor) and the current flowing through that resistor. Those two variables are represented algebraically with symbols, Vr for the voltage across the resistor, and Ir for the current flowing through the resistor.

It's important to remember that the voltage across the resistor, and the current through the resistor are related by Ohm's Law: Vr = RIr when the polarities are as shown below.

We need to be very precise when we consider Ohm's law because the polarities are very important.

  • Ohm's law holds - that is Vr = RIr - only when the current is defined positive flowing into the terminal that is labelled positive for the voltage.
  • We paraphrase that by saying that Ohm's law holds in the usual form whenever the arrow defining positive current flows into the "+" terminal (referring to voltage polarity definition).

Questions

Q11. Which is the correct expression for Ohm's law when polarities are defined as shown below?

Q12. Which is the correct expression for Ohm's law when polarities are defined as shown below?

Q13. Which is the correct expression for Ohm's law when polarities are defined as shown below?


Physical Resistors

While it is true that a piece of metal, like a wire for example, is a resistor of sorts, you need to know that today resistors are made with specific values, and they often take a common form. Typically they look like the one shown at the right - only they' be pretty small, maybe a half to three quarters of an inch long for the body.

A resistor is typically formed from some sort of resistive material and put into a cylindrical form. Usually the resistor will have a brownish body with several stripes painted on the resistor body. Those stripes are in a code that will tell you the value of the resistors (in ohms). Here's what's important.

The resistor shown above is 1000 ohms = 10x102

Notice how cleverly we put certain parts of the result in bold text and colored it. The bolded text corresponds to the stripes, and the colors are shown on the bold text. Here is the color code.

0 Black Black
1 Brown Brown
2 Red Red
3 Orange Orange
4 Yellow Yellow
5 Green Green
6 Blue Blue
7 Violet Violet
8 Gray Gray
9 White White

Given a resistor, to calculate the value of the resistance you use the three stripes. (If there are four stripes, just use the first three. The last stripe tells you how accurate the resistance value is.) Here is the algorithm.

  • The first stripe is the most significant digit, X, in XY x 10Z.
  • The second stripe is the next digit, Y, in XY x 10Z.
  • The third stripe is the exponent in XY x 10Z.
Here is an example/problem.


Measuring Resistance

In this section you'll learn a little about how to measure resistances. You'll need to have an ohmmeter, a digital multimeter or a data acquisition unit. When you use any of those instruments to measure a resistance, the same thing happens. It's just that a digital multimeter can make voltage and current measurements, while a data acquisition unit can measure frequency and temperatures.

We'll also assume that you're in a lab running these lessons and that you have a lab notebook that you are using. (You should always have a lab notebook for lab work!)

An ohmmeter measures resistance, and gives you a value of the measured resistance in ohms, kilohms or megohms. Many ohmmeters look like the following diagram.

There's an internal source that provides a voltage. That source may be a battery or a small power supply. The source drives a voltage divider - two resistors in series. One of those resistors is internal to the meter, and the other resistor is the resistor being measured. An internal meter measures the voltage across the resistance being measured and converts that voltage into a resistance reading. The resistance being measured is connected to the ohmmeter terminals, and the terminals are often colored black and red.

All you have to do to measure a resistance is to connect your resistor to the ohmmeter as shown at the right, and be sure that the ohmmeter (or DVM or DAU) is set to measure resistance. Don't get uptight about which lead goes on which end of the resistor. It doesn't matter. (The resistor is a "bilateral" element and should be the same either way!)

Here's the way you connect the ohmmeter (or digital voltmeter or data acquisition unit) to the resistor. Here we're using the same resistor as was used in the questions above. The ohmmeter shown here includes all of the circuitry shown above including a power supply or battery and an internal resistance. To measure the resistance it applies a small voltage across the resistance.

At this point, you are ready to start the first laboratory exercise on resistors.


Physical Resistors - Calculating Resistance From Geometry

The resistance of a resistor is determined by several physical properties of the resistor. We're going to limit ourselves to resistors that have a constant cross section - like a wire. Here are the properties.

  • The geometry of the conductor, including:
    • The length, L
    • The cross-sectional area, A
  • A constant of the material called the resistivity, r.
If you have those quantities, then the resistance is given by:

R = rL/A


What If Questions

You may be tempted to conclude that there are no serious "What If?" questions for resistors. Actually, there are many questions about these devices. Note the following characteristics of resistors.

  • Resistors have voltage directly proportional to the current. That's true at every instant of time and for every frequency. Is it possible to have a situation in which voltage and current are not proportional?
    • In diodes - and many other devices, current and voltage are nonlinearly related. There are many devices in which the relationship is not proportional or linear.
  • The voltage across a resistor and the current through the resistor depend upon the values at the same time. Is it possible to have other kinds of relationships?
    • In a capacitor, we have i(t) = Cdv(t)/dt.
    • In an inductor, we have v(t) = Ldi(t)/dt.
    • Capacitors and inductors have voltage and current related to derivatives! That's really a different situation because it means you have to learn how to solve differential equations ot predict behavior of circuits with these components. That's a whole new kettle of fish.
  • A resistor is a two-terminal device. Transistors have three terminals. That means that the analysis is much more complicated.
And, if Ohm hadn't discovered his famous law - and lost his job and been blackballed for ten years - you wouldn't be reading this now.


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