practical industrial electronics for engineers and technicians

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Technology Training that works Technology Training that Works www.idc-online.com/slideshare Practical Industrial Electronics for Engineers and Technicians

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Industrial electronics has become an integral part of our businesses. A working knowledge of electronics has now become a prerequisite for efficiency in the work place. This two-day workshop will 'demystify' the world of electronics to you and equip you to understand, identify and confidently troubleshoot electronic problems. You will gain the vital knowledge that you need to: multi-skill, reduce down-time, save your company money, and secure your value in the workplace. You will learn the latest trends and techniques in the fastmoving field of industrial electronics. WHO SHOULD ATTEND? All engineering, operations or management personnel who are directly or indirectly involved with electronics controls Anyone whose work requires the use of electronic equipment Maintenance technicians, electricians, foremen and engineers Mechanical and chemical engineers, operators and personnel who need electronics knowledge Those involved with the installing, programming, maintaining and purchasing of electronic control equipment Those who want to improve their understanding and capabilities in electronic technology Those who wish to be able to multi-skill into electronics maintenance technicians, electricians, foremen and engineers MORE INFORMATION: http://www.idc-online.com/content/practical-industrial-electronics-engineers-and-technicians-11

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Page 1: Practical Industrial Electronics for Engineers and Technicians

Technology Training that worksTechnology Training that Workswww.idc-online.com/slideshare

Practical Industrial Electronics for Engineers and Technicians

Page 2: Practical Industrial Electronics for Engineers and Technicians

Technology Training that worksTechnology Training that Workswww.idc-online.com/slideshare

The Bohr model of an atom

• An atom have a planetary type of structure.

• The atom consists from a nucleus and electrons, orbiting around the nucleus.

• The nucleus consists from protons and neutrons.

Page 3: Practical Industrial Electronics for Engineers and Technicians

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The two simplest atoms

Page 4: Practical Industrial Electronics for Engineers and Technicians

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Atomic number

• The atomic number equals the number of protons in the nucleus.

• A balanced atom has equal number of protons and electrons.

Page 5: Practical Industrial Electronics for Engineers and Technicians

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Electron shells

• The electrons do not orbit the nucleus of an atom at random distances.

• The distances, at which electrons orbit the nucleus are precisely defined into energy bands, called shells.

Page 6: Practical Industrial Electronics for Engineers and Technicians

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Valence

• The outermost shell or energy level that contains electrons is known as the valence level of that atom.

• The number of electrons in the outer level is known as the valence number of that atom.

• The electrons in this level are called valence electrons.

Page 7: Practical Industrial Electronics for Engineers and Technicians

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Ionization

• The process of losing a valence electron is called ionization.

• Free electrons may join positive ions turning them again into neutral atoms. This process is called recombination.

Page 8: Practical Industrial Electronics for Engineers and Technicians

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Conductors

• A conductor is a material that easily conducts electrical current.

• Atoms with a low valence number (1,2 and 3) make very good conductors of electricity.

Page 9: Practical Industrial Electronics for Engineers and Technicians

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Conductor structure

Page 10: Practical Industrial Electronics for Engineers and Technicians

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Insulators

• An insulator is a material that does not conduct electrical current.

• Atoms of insulating materials consist of at least 5 valence electrons.

Page 11: Practical Industrial Electronics for Engineers and Technicians

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Energy diagrams

Page 12: Practical Industrial Electronics for Engineers and Technicians

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Conductor with current flowEMF

Page 13: Practical Industrial Electronics for Engineers and Technicians

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Current, voltage and power relationship

V = W

Q

– V is emf in volts (V)– W is work done in joules (J) – Q is charge in coulombs (C)

Page 14: Practical Industrial Electronics for Engineers and Technicians

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Two conditions for the electrical current to flow:

• External source of emf must be available.

• The electrical circuit must be closed.

V No Current F low

R

Page 15: Practical Industrial Electronics for Engineers and Technicians

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Resistance and resistivity

• The quality that describes how much the material counteracts the electrical current flowing through it is called electrical resistance.

• Resistivity represents the electrical resistance of one cubic centimeter of the given substance.

Page 16: Practical Industrial Electronics for Engineers and Technicians

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Electrical power• Electrical power is equal to the work done for

certain time and can be expressed with the formula:

P = W

t– P is the electrical power in watts– W is work done in joules (J) – t is the time in seconds (s)

Page 17: Practical Industrial Electronics for Engineers and Technicians

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Direct current

• If the voltage source is a constant polarity supply than the current always flows in one direction. For this reason it is called dc (direct current).

• The voltage from this source is called dc voltage.

• DC can be produced from batteries and DC generators.

Page 18: Practical Industrial Electronics for Engineers and Technicians

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A battery

• A battery is a device that creates a potential difference on its two terminals by means of chemical reaction.

• Each battery consists of one or more units, called cells.

• The cell contains electrolytes that take part in the chemical reaction.

Page 19: Practical Industrial Electronics for Engineers and Technicians

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Memory effect

• This effect occurs when the battery is not fully discharged every time when it is used.

• Then the battery “remembers” only the capacity rate at which it was lastly used.

• The memory effect can be overcome with deep cycling.

Page 20: Practical Industrial Electronics for Engineers and Technicians

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Alternating current (ac)

• The alternating current (ac) constantly reverses its direction of flow.

• To generate and to transmit ac is much easier and cheaper than dc.

• It is much easier to transform ac into dc, than vice versa.

Page 21: Practical Industrial Electronics for Engineers and Technicians

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Magnitude of the induced emf

e = B l v

– e is the emf, induced across the conductor– B is the flux density,.– l is the conductor’s length,– v is the conductor’s speed

Page 22: Practical Industrial Electronics for Engineers and Technicians

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Speed of conductor

v = vr sin

– vr is conductor’s speed of rotation,

– sin is the angle between the speed (v) and the magnetic flux (B).

Page 23: Practical Industrial Electronics for Engineers and Technicians

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Equation for the sine wave

e = B l vr sin

– e is the emf, induced across the conductor– B is the flux density– l is the conductor’s length

– vr is conductor’s speed of rotation

– sin is the angle between the speed (v) and the magnetic flux (B).

Page 24: Practical Industrial Electronics for Engineers and Technicians

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Sine wave

Page 25: Practical Industrial Electronics for Engineers and Technicians

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Generating sine emf in a loop

• The loop represents two conductors, connected in series

e L = 2 B l vr sin

– eL is the total emf, induced in the loop

Page 26: Practical Industrial Electronics for Engineers and Technicians

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Period • A period is the smallest interval of time taken for the sine

wave to complete one full cycle. • When the cycle is complete, the sine wave begins to

repeat the quantities of the current in the same sequence.

Page 27: Practical Industrial Electronics for Engineers and Technicians

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Frequency

• The frequency depends on the number of full periods, contained in one second.

f = 1

T– f is the frequency of the sine wave,– T is the period of the sine wave

Page 28: Practical Industrial Electronics for Engineers and Technicians

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A peak value

Page 29: Practical Industrial Electronics for Engineers and Technicians

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A peak-to-peak value

Page 30: Practical Industrial Electronics for Engineers and Technicians

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An average value

Page 31: Practical Industrial Electronics for Engineers and Technicians

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A root-mean-square value

root-mean-square value is equal to the value of a direct current, producing the same amount of heat, in the same load for the same time, as an alternating current.

I = Ip = 0.707 Ip

2

V = Vp = 0.707 Vp

2

Page 32: Practical Industrial Electronics for Engineers and Technicians

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