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2.01 - 2.10
FUNDAMENTALS OF HIGH
 FREQUENCY CURRENTS

     TEACHER : Dr. RINKU SHAH (PT)
                  Dr. KAJAL PATEL (PT)
 VERIFIED BY : Dr. ASHOK CHAUDHARY (PT)
 VALIDATED BY : Dr. POONGUNDRAN P. (PT)
MAGNETISM


2.01 to 2.10 Fundamentals of high frequency currents   2
• A magnet is an object which exhibits certain
  properties.
• For example, when free to rotate, it will align
  itself in the North—South direction.
• It also has the power to attract, and produce
  magnetism in, certain other materials.
• So, A piece of substance, which possesses the
  property of attracting small pieces of iron
  towards, it is called a magnet.
           2.01 to 2.10 Fundamentals of high frequency currents   3
• If the property of magnetism occurs naturally
  the magnet is known as a Natural magnet.
• It is possible artificially to induce magnetism
  by rubbing the given piece of substance with
  magnets.
   – The magnet thus produced is called an
      Artificial Magnet.

           2.01 to 2.10 Fundamentals of high frequency currents   4
The molecular theory of
               magnetism
• No matter how many times a magnet is
  divided, it will always present a North and a
  South pole.
• This phenomenon could conceivably be
  carried on down to molecular level, where it is
  thought that the revolving electrons produce
  a North and a South pole for each molecule,
  giving so-called ‘Molecular Magnets’.

           2.01 to 2.10 Fundamentals of high frequency currents   5
• In a non-magnetized state, these molecular
  magnets are arranged in a haphazard way and
  cancel out one another’s effects.
• In the magnetized state, the molecular
  magnets are ordered so that one end of the
  piece of metal exhibits a North pole and the
  other a South.

          2.01 to 2.10 Fundamentals of high frequency currents   6
• In magnetized materials such as steel, the
  friction between the molecules is great and the
  ordered magnetic effect is retained, giving a
  permanent magnet.
• Heating or banging will, however, disrupt the
  order and so the magnetism will be lost.


          2.01 to 2.10 Fundamentals of high frequency currents   7
• Haphazard arrangement of molecular
  magnets.

         2.01 to 2.10 Fundamentals of high frequency currents   8
• Ordered arrangement of molecular magnets


         2.01 to 2.10 Fundamentals of high frequency currents   9
• In a material such as soft iron there is little
  friction between the molecules, so although they
  can easily be influenced into an ordered pattern,
  this pattern will also be lost very easily.
• Thus soft iron only forms temporary magnets
• The magnetic effect of a wire carrying an electric
  current can be used to create an electromagnet,
  which exists only for as long as current flows.
            2.01 to 2.10 Fundamentals of high frequency currents   10
• Magnetization by contact.

   2.01 to 2.10 Fundamentals of high frequency currents   11
• The magnetic field around a bar magnet.

          2.01 to 2.10 Fundamentals of high frequency currents   12
Magnetic Poles

• The points inside the magnet, where
  attraction is maximum are called poles.
• Every magnet has two poles: north pole and
  south pole.
• A freely suspended magnet sets itself in the
  direction of geographic north and south.


          2.01 to 2.10 Fundamentals of high frequency currents   13
• North pole: The end of the magnet pointing
  towards north is called north seeking pole or
  north pole.
• South pole: The end of the magnet pointing
  towards south is called south seeking pole or
  south pole.


          2.01 to 2.10 Fundamentals of high frequency currents   14
• In a magnet the unlike poles attract each
  other and like poles repel each other.
• Two magnets one of which is suspended
  comes closer to the other when their opposite
  poles are kept nearer, whereas it moves apart
  when their like poles are kept nearer.


          2.01 to 2.10 Fundamentals of high frequency currents   15
Properties of a magnet


1. Setting in a North—South direction As the
   Earth itself is a giant magnet, the Earth’s
   magnetic field will influence a suspended
   magnet so that one of its poles (ends) will
   settle in the direction of the Earth’s North
   Pole.


           2.01 to 2.10 Fundamentals of high frequency currents   16
2. Like magnetic poles repel one another North
   repels North and South repels South.
• Unlike magnetic poles attract one another,
   i.e. North attracts South and South attracts
   North.



          2.01 to 2.10 Fundamentals of high frequency currents   17
3. Transmission of properties: A magnet can
   produce properties of magnetism in suitable
   materials.
• As one pole of a bar magnet is stroked along the
   material; all the opposite poles of the molecular
   magnets are attracted towards it so that the
   object is magnetized.
• The end that the magnet leaves will have the
   pole opposite to that used to induce the effect.
            2.01 to 2.10 Fundamentals of high frequency currents   18
• A magnet may also produce a magnetic effect
  in an object without contact between them
  (magnetic induction).
• Once again, it is the influence of the magnet
  over the molecular magnets of the susceptible
  materials which produces the magnetic effect.


          2.01 to 2.10 Fundamentals of high frequency currents   19
4. Attraction of suitable materials Magnets
   attract certain materials.
• This effect is produced by magnetic
   induction.



          2.01 to 2.10 Fundamentals of high frequency currents   20
5. A magnetic field: This is the area or zone of
   influence around a magnet in which its
   magnetic forces are apparent.




           2.01 to 2.10 Fundamentals of high frequency currents   21
• This field may be considered as being made up
  of magnetic lines of force which have the
  following properties:
  a) They travel from North to South, which is the
     path a free North Pole would take.
  b) They attempt to take the shortest route possible
     but repel one another so that they in fact become
     curved.
  c) They travel more easily through some materials,
     e.g. metals, than through others.
           2.01 to 2.10 Fundamentals of high frequency currents   22
Types of Magnet
Magnets are of two types
• Natural magnets: The magnets found in
  nature are called natural magnets. These
  magnets are weak and shapeless.
• Artificial magnets: Man made magnets are
  called artificial mans. These magnets are
  strong and of different shapes.
• They may be bar shaped, horseshoe shaped,
  magnetic needles, magnetic compass, etc.
          2.01 to 2.10 Fundamentals of high frequency currents   23
Types of Artificial Magnets


1. Temporary magnets: Magnetism of these
   magnets is temporary. It is made of soft iron.
2. Permanent magnet: Magnetism of these
   magnets is permanent. It is made up of steel,
   nickel and cobalt.



           2.01 to 2.10 Fundamentals of high frequency currents   24
Electromagnetism


  2.01 to 2.10 Fundamentals of high frequency currents   25
• Electromagnetism is one of the four
  fundamental forces known to exist in the
  universe.
• An electromagnet consists of a coil of wire
  wound onto a soft iron bar.
• When a current passes through the wire it
  magnetizes the bar by induction.

           2.01 to 2.10 Fundamentals of high frequency currents   26
• As soon as the current is put off, the magnetic
  effect is lost.
• Wires carrying an electric current produce
  magnetic field around a straight wire in the
  form of concentric circles with the wire at
  their center.


           2.01 to 2.10 Fundamentals of high frequency currents   27
• A coil of wire produces a field somewhat
  similar to that of a bar magnet, with the main
  difference being that in electromagnetism a
  uniform field is produced inside it.
• This uniformity of field is used as an
  advantage in SWD application.



           2.01 to 2.10 Fundamentals of high frequency currents   28
• A coil of wire produces a field somewhat
  similar to that of a bar magnet, with the main
  difference being that in electromagnetism a
  uniform field is produced inside it. This
  uniformity of field is used as an advantage in
  SWD application.



           2.01 to 2.10 Fundamentals of high frequency currents   29
Electromagnetic induction
• Electromagnetic induction is the means by
  which electricity is produced from magnetism
  (and vice-versa).
• It is the result of interaction between a
  conductor and magnetic lines of force.
• An EMF is produced in the conductor by the
  magnetic lines of force surrounding a magnet,
  without contact between the magnet and the
  conductor.
          2.01 to 2.10 Fundamentals of high frequency currents   30
Electromagnetic induction


• The factors essential to electromagnetic
  induction are:
1. Conductor
2. Magnetic lines of force
3. Relative movement of 1 and 2


          2.01 to 2.10 Fundamentals of high frequency currents   31
Electromagnetic induction
• If the conductor is part of a closed circuit, the
  magnetic lines of force produce an EMF which
  causes movement of the electrons in the
  conductor.
• This can be shown with an ammeter connected
  across a coil of wire When a magnet is moved
  into the coil, the magnetic lines of force cut
  across the conducting wire of the coil and cause
  movement of electrons in the coil.
           2.01 to 2.10 Fundamentals of high frequency currents   32
Electromagnetic induction

• These electrons repel adjacent electrons and
  so on, and a current is set up in the circuit.
  Movement of the ammeter needle, indicating
  current flow, will be seen only when either
  the magnet or the coil is moving. If the
  magnetic lines of force are stationary relative
  to the coil of wire, there is no induction.


           2.01 to 2.10 Fundamentals of high frequency currents   33
• Electromagnetic induction also occurs if the
  magnetic field used is that surrounding a coil
  Of wire.
• The principles are the same. There must be
  movement of the magnetic field relative to
  the conductor.



           2.01 to 2.10 Fundamentals of high frequency currents   34
• This may be achieved by using an alternative
  current in the primary coil which causes the
  magnetic field to build up, fall, then build up
  in the opposite direction, then fall, etc.
• The current builds up to a maximum positive
  value and then falls to zero. It then drops to a
  maximum negative value before returning to
  zero. This rise and fall of current produces
  movement of the magnetic lines of force.
           2.01 to 2.10 Fundamentals of high frequency currents   35
• In practice, the conductor in which the EMF is
  induced is usually a coil of wire, while the
  magnetic field used to induce the EMF is that
  of a permanent magnet or a current-carrying
  coil of wire.



          2.01 to 2.10 Fundamentals of high frequency currents   36
• Movement of one of these relative to the
  other is achieved either by spinning the
  conductor in the magnetic field, as in a
  dynamo, or by varying the intensity of current
  in the coil of wire, as in a transformer



          2.01 to 2.10 Fundamentals of high frequency currents   37
The direction of the
                  induced EMF

• The direction in which the magnetic lines of
  force move relative to the conductor affects
  the direction in which the induced current
  flows. This can again be seen by using the bar
  magnet and coil.



           2.01 to 2.10 Fundamentals of high frequency currents   38
The direction of the
                 induced EMF
• As the magnet is moved into the coil, the
  ammeter needle deflected in one direction.
• As it is withdrawn, deflection occurs in the
  opposite direction, thus demonstrating that
  the direction of current flow changes with a
  reversal of movement of the magnetic field.



          2.01 to 2.10 Fundamentals of high frequency currents   39
The direction of the
                  induced EMF
• The same is true when the inducing magnetic
  field is that surrounding a current-carrying coil
  of wire.
• As the current rises and the magnetic lines of
  force move out, thus cutting the conductor,
  deflection of the ammeter needle occurs in
  one direction.


           2.01 to 2.10 Fundamentals of high frequency currents   40
The direction of the
                  induced EMF
• As the current drops to zero, the magnetic
  lines of force move back in towards the
  primary coil. The direction of movement of
  these lines of force is now reversed, and so is
  the direction of the induced current indicated
  by the ammeter.




           2.01 to 2.10 Fundamentals of high frequency currents   41
The direction of the
                 induced EMF

• This result is often quoted as Lenz’s law,
  which states that the direction of the induced
  EMF is such that it tends to oppose the force
  producing it.




          2.01 to 2.10 Fundamentals of high frequency currents   42
The strength of the induced
                  EMF


• This depends upon two factors:
1. the rate of change of the magnetic field
2. the inductance of the conductor




          2.01 to 2.10 Fundamentals of high frequency currents   43
1 The rate of change of
            the magnetic field

• The more rapid the movement of the
  permanent magnet and the stronger the
  magnet used, the greater is the rate at which
  the magnetic lines of force cut the conductor
  and the greater the induced EMF.



          2.01 to 2.10 Fundamentals of high frequency currents   44
1 The rate of change of
             the magnetic field

• In the case of a current-carrying coil of wire, if
  the frequency of current is increased (and
  hence the rate of rise and collapse of the
  magnetic field), a stronger EMF is induced.




           2.01 to 2.10 Fundamentals of high frequency currents   45
2 The inductance of the
                 conductor
• Inductance is the ability of a conductor to
  have a current induced in it. Inductance is
  measured in henries.
• Inductance is constant for any particular
  conductor, but high inductance can be
  designed into a conducting coil by
  incorporating the following principles:

           2.01 to 2.10 Fundamentals of high frequency currents   46
2 The inductance of the
                 conductor
1. Using many turns of wire in the coil
2. Placing the turns close together
3. Winding the coil onto a soft iron core
• This ensures that the magnetic lines of force
  cut the maximum number of coils in the
  conductor and thus induce a strong EMF into
  it.


          2.01 to 2.10 Fundamentals of high frequency currents   47
LAWS


2.01 to 2.10 Fundamentals of high frequency currents   48
Faraday’s Law of
        Electromagnetic Induction


• Faraday’s laws deal with the induction of EMF
  in an electrical circuit, when magnetic flux
  linked with the circuit changes.




          2.01 to 2.10 Fundamentals of high frequency currents   49
Faraday’s Law of
        Electromagnetic Induction
• Whenever magnetic flux linked with a circuit
  changes, an EMF is induced in it.
• An induced EMF exists in the circuit, so long as
  the change in magnetic flux linked with it
  continues.
• The induced EMF is directly proportional to
  the negative rate of change of magnetic flux
  linked with the circuit.

           2.01 to 2.10 Fundamentals of high frequency currents   50
Lenz’s Law



• The law states that the direction of the
  induced EMF (current) is such that it opposes
  the very cause, which produces it.




          2.01 to 2.10 Fundamentals of high frequency currents   51
Fleming’s Right Hand Rule

• It gives us the direction of the induced EMF
  (current), in a conductor moving in a magnetic
  field. It states that, if the thumb, index and
  middle fingers of the right hand are stretched
  mutually perpendicular, then thumb indicates
  motion, index finger indicates the direction of
  the field and middle finger indicates the
  direction of induced current.


           2.01 to 2.10 Fundamentals of high frequency currents   52
Mutual Induction

• Mutual induction is said to occur when an
  EMF is induced in an adjacent conductor by
  the magnetic field set-up around a coil of wire
  carrying a varying current. In a transformer
  and in physiotherapy this principle is very
  much used in the electrotherapeutic
  modalities, e.g. SWD.


           2.01 to 2.10 Fundamentals of high frequency currents   53
Self Induction


• Self induction occurs with in a coil carrying a
  varying current. A magnetic field is set-up
  around each turn of wire.
• As the current increases, the magnetic lines of
  force move out, cutting adjacent turns of wire
  and thus inducing an EMF in them.


           2.01 to 2.10 Fundamentals of high frequency currents   54
Self Induction

• Following Lenz’s law, the direction of the
  induced EMF will be opposite to the force (or
  current) producing it.
• Therefore, the induced EMF is in the opposite
  direction to the main current and so opposes
  its rise. Self induced EMF of this type is
  therefore, called back EMF.


          2.01 to 2.10 Fundamentals of high frequency currents   55
Self Induction
• A similar sequence of events occurs when the
  primary current starts to fall. The magnetic
  field now collapses and the lines of force
  move back in, cutting adjacent turns of wire
  but in the opposite direction from before.
• Consequently, the induced EMF is also in the
  opposite direction and flows forward as the
  forward EMF.


          2.01 to 2.10 Fundamentals of high frequency currents   56
Self Induction

• The overall effect of back and forward EMF is
  to retard the rate of rise of current and
  prolong its fall.




          2.01 to 2.10 Fundamentals of high frequency currents   57
Choke coil

• It is a device included in the circuit to produce
  self induced EMF, maintaining a smooth flow
  of current. It is of two types, i.e. low
  frequency choke coil and high frequency
  choke coil.



           2.01 to 2.10 Fundamentals of high frequency currents   58
Low Frequency Choke Coil
                Choke coil
• This consists of many
  turns of insulated
  wire, wound on a
  laminated soft iron
  frame, usually on the
  central bar of a
  rectangular frame


            2.01 to 2.10 Fundamentals of high frequency currents   59
Low Frequency Choke Coil
              Choke coil
• When a current, which varies in intensity, is
  passed through the coil, magnetic lines of
  force are set-up, which cut the turns of wire
  and induce EMF in them.
• There are many turns of wire, so the coil has
  considerable inductance and self-induced EMF
  is large.



          2.01 to 2.10 Fundamentals of high frequency currents   60
Low Frequency Choke Coil
               Choke coil

• The core serves to concentrate the magnetic
  field, it is made of soft iron, so that it is easily
  magnetized and de-magnetized, and is
  laminated to prevent eddy currents.




            2.01 to 2.10 Fundamentals of high frequency currents   61
High Frequency Choke
                   Coil
• A high frequency current varies very rapidly in
  intensity so tend to produce a considerable
  self-induced EMF.
• Consequently, it is unnecessary to have many
  turns of wire, in a high frequency choke coil,
  or to wind them on a soft iron core.
• The coil usually consists of several turns of
  insulated wire wound on the bobbin of some
  non-conducting material.
           2.01 to 2.10 Fundamentals of high frequency currents   62
Uses of choke coil

• To even out the variations in the intensity of
  the current, providing a smooth current flow:
The self-induced EMF, which is set-up when a
  varying current is passed through a choke coil,
  retards the rise of current to a maximum, and
  prolongs the current flow, when the intensity
  is falling, there by maintaining an even flow of
  current.

           2.01 to 2.10 Fundamentals of high frequency currents   63
Uses of choke coil

• To prevent the flow of a high frequency
  current and allow the passage of the low
  frequency one:
When a high frequency current is passed
  through a choke coil, the inductive reactance
  is considerable, there by retarding the flow of
  such a current,



           2.01 to 2.10 Fundamentals of high frequency currents   64
Uses of choke coil



when a low frequency current is passed, the
 impedance to current flow is very less, due to
 which the choke coil serves the above
 function.




          2.01 to 2.10 Fundamentals of high frequency currents   65
Eddy Current

• Any conductor lying in a
  varying magnetic field has
  an EMF induced in it. If
  the conductor is solid, the
  magnetic lines of force
  passing through it set-up
  circular currents called
  eddy currents

           2.01 to 2.10 Fundamentals of high frequency currents   66
Eddy Current

• In the figure shown below,
  the solid conductor ‘B’ is
  present in the varying
  magnetic field which
  produces the eddy currents
  in it shown by the arrow
  pointing up and down.


          2.01 to 2.10 Fundamentals of high frequency currents   67
Eddy Current


• These eddy currents are perpendicular to the
  magnetic lines of force and produce heating
  effect in tissues in accordance with Joules




          2.01 to 2.10 Fundamentals of high frequency currents   68
Transformer


2.01 to 2.10 Fundamentals of high frequency currents   69
• It is a device used for changing low alternating
  voltage at high current. It changes the
  alternating voltage without the loss of energy.




           2.01 to 2.10 Fundamentals of high frequency currents   70
Types of Transformer


• Broadly the transformers are divided into
  three types
1. static transformer
2. variable transformer
3. autotransformer


          2.01 to 2.10 Fundamentals of high frequency currents   71
Static Transformer


• The static transformer is based on the
  principles of electromagnetic induction, and is
  used to alter voltage of an alternating current
  and to render the current earth free.




           2.01 to 2.10 Fundamentals of high frequency currents   72
Static Transformer-
                   construction
• It consists of two coils
  of insulated wire, the
  primary and the
  secondary coils,
  wound on a laminated
  soft iron core.



           2.01 to 2.10 Fundamentals of high frequency currents   73
Static Transformer-
                  construction
• The coils are completely insulated from each
  other and one usually contains more turns of
  wire than the other.
• The frame is often rectangular in shape and
  the coils may be wound on opposite bars of
  the frame or one on top of the other on a
  central bar.


          2.01 to 2.10 Fundamentals of high frequency currents   74
Static Transformer-
                      working
• An alternating current is passed through the
  primary coil and sets up a varying magnetic
  field, which cuts the secondary coil and
  induces an EMF in it.
• It is essential that the primary current varies
  in intensity, otherwise there is no movement
  of the magnetic field relative to the conductor
  and no EMF is induced in the secondary coil.

           2.01 to 2.10 Fundamentals of high frequency currents   75
Static Transformer-
                      working
• There is no electrical conduction between the
  primary and the secondary coils, the energy
  being transmitted from one to the other by
  electromagnetic induction.
• The core serves to concentrate the magnetic
  field and is made of soft iron, as this material
  is easily magnetized and de magnetized. It is
  laminated to prevent eddy currents.


           2.01 to 2.10 Fundamentals of high frequency currents   76
Static Transformer-
                     functions
1. Alters the voltage of an alternating current
• The EMF induced in the secondary coil
   depends upon the number of turns of wire it
   has, relative to the primary coil. Depending
   on this number of turns, the transformers
   can be classified as:
  – Step up transformer
  – Step down transformer
  – Even ration transformer
          2.01 to 2.10 Fundamentals of high frequency currents   77
Step up transformer

• If the number of turns in
  the secondary are more
  than that of the primary,
  the voltage developed in
  the secondary will be
  increased or stepped up.
  Such a device is called as
  step up transformer.

            2.01 to 2.10 Fundamentals of high frequency currents   78
Step down transformer
• If the secondary coil has
  fewer turns than the
  primary, then the EMF,
  or voltage in the
  secondary will be less
  than in the primary, i.e.
  it is stepped down. Such
  an arrangement
  produces a step down
  transformer.
            2.01 to 2.10 Fundamentals of high frequency currents   79
Even ratio transformer

• If the number of turns in the primary and
  secondary coils are same, the voltage in the
  primary is same as that of the secondary. Such
  a device is called even ratio transformer.
• It is important to note that, the electrical
  power in both the primary and the secondary
  circuits are always the same.


          2.01 to 2.10 Fundamentals of high frequency currents   80
Even ratio transformer


• Power is measured in watts (volts x ampere),
  so the quantity watts x ampere must be same
  for both the primary and secondary coils, i.e.
  any change in voltage must be accompanied
  by a change in current.



          2.01 to 2.10 Fundamentals of high frequency currents   81
Static Transformer-
                      functions

2. Renders a current earth free
• The mains electricity is produced by the
  dynamo, and the consumer is supplied with a
  wire at high potential, called the live wire, and
  a wire at zero potential connected to earth,
  called the neutral wire.


           2.01 to 2.10 Fundamentals of high frequency currents   82
• Most electrical
  apparatus works on a
  current, which flows
  from the live wire,
  through the
  apparatus, to the
  neutral wire and
  earth.


           2.01 to 2.10 Fundamentals of high frequency currents   83
• If an accidental connection is made between
  live wire and earth, current will flow along it.
• If this connection were made through a
  person, they would then receive an earth
  shock, as the current flows through them to
  earth.


           2.01 to 2.10 Fundamentals of high frequency currents   84
• The static transformer
  reduces this danger by
  using electromagnetic
  induction, to transfer
  the electrical energy
  into the secondary coil
  where earth plays no
  part in the circuit.

           2.01 to 2.10 Fundamentals of high frequency currents   85
• The effect on the secondary coil of the
  magnetic field around the primary is to cause
  electrons to move around the secondary
  circuit, but not to leave it. Earth plays no part
  in the secondary circuit, because, even if an
  earth connection is made with it, electrons
  will not leave the circuit, but will continue to
  flow around it

           2.01 to 2.10 Fundamentals of high frequency currents   86
• This is an important safety factor, and that all
  currents applied to patients are rendered
  earth free by using a static transformer.




           2.01 to 2.10 Fundamentals of high frequency currents   87
Variable Transformer


• It consists of a
  primary and
  secondary coil, but is
  constructed so that
  one of them can be
  altered in length.


           2.01 to 2.10 Fundamentals of high frequency currents   88
Variable Transformer

• The primary coil has a number of tapings
  taken from it and a movable contact can be
  made on any one of these by turning a knob.
• The effect of decreasing the number of turns
  in the primary coil relative to the secondary is
  to cause a step up voltage in the secondary
  coil. In his way a very crude control of voltage
  is obtained.

           2.01 to 2.10 Fundamentals of high frequency currents   89
Autotransformer




• It consists of a single coil of wire with four
  contact points coming from it.




           2.01 to 2.10 Fundamentals of high frequency currents   90
Autotransformer


• It can be used as a step up, or a step down
  transformer. When used as the step up, CD is
  the primary coil and AB is the secondary coil.
  When used as the step down, AB is the
  primary and CD is the secondary coil.
  Although the autotransformer works on the


           2.01 to 2.10 Fundamentals of high frequency currents   91
Autotransformer


• Although the autotransformer works on the
  principles of electromagnetic inductions, it
  has the disadvantage that, it allows only a
  small step up, and does not render the
  current earth free.
• It is used in the starter circuit of ultraviolet
  lamp to strike the arc in the lamp.

           2.01 to 2.10 Fundamentals of high frequency currents   92
Diode & triode valves


    2.01 to 2.10 Fundamentals of high frequency currents   93
Valve

• Valve is a device, which transmits the flow in
  one direction only, common examples being
  that of the valves of heart, or vein.
• In electronics a thermionic valve is defined as
  a device allowing unidirectional flow of
  current.



           2.01 to 2.10 Fundamentals of high frequency currents   94
Valve

• There are various types of thermionic valves,
  which are named according to the number of
  electrodes they contain. They are:
  1. Diode valve
  2. Triode valve




          2.01 to 2.10 Fundamentals of high frequency currents   95
Diode valve

• This is the simplest form of thermionic valve,
  containing a cathode with a filament and an
  anode, enclosed in an evacuated glass tube.
• The valve may either be evacuated or may
  contain an inert gas at low pressure.




           2.01 to 2.10 Fundamentals of high frequency currents   96
Diode valve

• For the current to pass through the valve, the
  filament must be heated, causing emission of
  electrons by the process of thermionic
  emission & a PD when applied makes the
  plate (anode) positive in relation to the
  cathode.



           2.01 to 2.10 Fundamentals of high frequency currents   97
Diode valve

• The filament used can be directly or indirectly
  heating type and the anode plate is made
  from some metal, which does not allow
  thermionic emission readily and is in the form
  of a cylinder surrounding the cathode.



           2.01 to 2.10 Fundamentals of high frequency currents   98
Diode valve
• The directly heating filament is a loop of fine
  wire of thoriated tungsten (tungsten can
  tolerate repeated and cooling, allowing
  emission of electrons at low temperature)
• The indirectly heating filament is a fine loop of
  wire embedded in some insulated material
  and the whole device is surrounded by a
  metal cylinder from which thermionic
  emission takes place.
           2.01 to 2.10 Fundamentals of high frequency currents   99
Diode valve
• The electrons so emitted will be attracted by
  the positive anode constituting an electrical
  current across the device.
• When the applied PD is reversed, so that the
  plate (anode) is negative with respect to the
  cathode, no current flows through the device,
  indicating that the electrons can pass from
  cathode to plate, not in the reverse direction,
  i.e. the current can flow only in one direction.
           2.01 to 2.10 Fundamentals of high frequency currents   100
Diode valve
• The intensity of current that flows across the
  valve depends on the heating of the filament
  and on the PD between the filament and the
  plate.
• If more current is applied to the filament
  causing increased heating of the same, it will
  emit more number of electrons and this when
  combined with an increase in PD, makes
  available greater force to attract the
  electrons.
          2.01 to 2.10 Fundamentals of high frequency currents   101
Diode valve

• And there by increasing
  the current flow across the
  valve. In a diode there are
  the filament circuit and
  the anode circuit.
• The diode is symbolically
  represented and three
  dimensionally as in Figure

            2.01 to 2.10 Fundamentals of high frequency currents   102
Triode valve

• The triode valve is a device that contains three
  electrodes viz. cathode, grid, and the anode.
• The grid, whose potential can be altered, is
  placed between the cathode and the anode.
• The grid, which surrounds the filament, may
  consist of a metal cylinder, perforated to
  allow the electrons to pass through, or may be
  a spiral of metal wire.

           2.01 to 2.10 Fundamentals of high frequency currents   103
Triode valve

• A lead from the grid is brought to a pin
  outside the base of the valve, necessitating
  four pins, i.e. two for the filaments, one for
  the grid and one for the anode.
• When the filament will be heated as like the
  diode, current passes from the valve in one
  direction only, i.e. from plate to cathode.


           2.01 to 2.10 Fundamentals of high frequency currents   104
Triode valve
• If the grid is uncharged, it has no effect on the
  current flow.
• If the grid is given with a negative charge from
  the outside source, it repels electrons, either
  causing a reduction of current flow, or
  resulting in complete cessation of current
  flow.
• If however, the grid is given a positive charge,
  the electrons can pass and the current flows.
           2.01 to 2.10 Fundamentals of high frequency currents   105
Triode valve
• The charges applied to the grid from the
  external source are called as grid bias.
• As the grid lies close to the cathode, than the
  anode, the charges on the grid has a greater
  influence, on the flow of current than a similar
  charge on the anode.
• The flow of current across the triode valve can
  be regulated by adjusting the bias of the grid.

           2.01 to 2.10 Fundamentals of high frequency currents   106
Triode valve
• The triode valve is represented symbolically
  and three dimensionally as in Figure




          2.01 to 2.10 Fundamentals of high frequency currents   107
Uses of a triode valve
• Used for the production of interrupted
  current and other muscle stimulating
  currents.
• Used for the production of high frequency
  currents in conjunction with a condenser and
  inductance.
• It is not used as a rectifier, but rectifies the
  current that passes through it.
• It is used as a switch.
           2.01 to 2.10 Fundamentals of high frequency currents   108
Semiconductors


 2.01 to 2.10 Fundamentals of high frequency currents   109
• Semiconductors are usually metals, which
  because of thermal agitations, or addition of
  impurities, have electrons free to conduct
  current.
• A semiconductor can either be of n-type, or p-
  type.


          2.01 to 2.10 Fundamentals of high frequency currents   110
• In a n-type semiconductor, there is an excess
  of electron, which carries current, where as in
  a p-type, the deficiency of electron give rise to
  positive hole, due to which current flow
  occurs.
• If a n-type and a p-type semiconductors are
  fused together, electrons can only pass in the
  n—>p direction, and the semiconductor
  therefore acts as a valve.
           2.01 to 2.10 Fundamentals of high frequency currents   111
N-type, Semiconductor
• An atom of silicon with atomic number 14, has
  4 electrons in the outer shell, and in a crystal
  of silicon these are held in forming bonds with
  neighboring atoms, so that there are no free
  electrons to transmit an electric current.
• When certain other materials such as
  phosphorous (atomic number 15, with 5
  electrons outside) are added to silicon it
  transmits current.
           2.01 to 2.10 Fundamentals of high frequency currents   112
2.01 to 2.10 Fundamentals of high frequency currents   113
• When silicon and phosphorous form covalent
  bonds, four electrons of phosphorus make
  bond with four electrons of silicon, leaving
  behind one free electron in the phosphorous
  which are not held in bond with other atoms,
  therefore carrying current, when connected
  with a source in the same way like the
  conductors.
• Such a material is called n-type
  semiconductor.
          2.01 to 2.10 Fundamentals of high frequency currents   114
2.01 to 2.10 Fundamentals of high frequency currents   115
2.01 to 2.10 Fundamentals of high frequency currents   116
P-type Semiconductor
• When silicon is added with certain other
  substances such as aluminium with an atomic
  number 13, the three outer electrons in the
  aluminium atom, makes bond with three
  electrons in the outer orbit of silicon, whereas
  for the 4th electron of silicon, there is no
  electron available on the outer orbit of
  aluminium, creating an electron deficiency
  called hole.
           2.01 to 2.10 Fundamentals of high frequency currents   117
• When a PD is applied to such a material,
  electrons move from some of the atoms into
  these unoccupied bonds or holes nearer to
  the positive poles, so that as the electrons
  move away from the negative towards the
  positive, the holes move from the positive
  towards the negative, constituting a flow of
  current.

          2.01 to 2.10 Fundamentals of high frequency currents   118
• The movement of positive holes from positive
  towards negative is equivalent to the
  movement of electrons from negative to
  positive.
• The material that transmits current in this
  manner is called a p-type semiconductor.


          2.01 to 2.10 Fundamentals of high frequency currents   119
2.01 to 2.10 Fundamentals of high frequency currents   120
2.01 to 2.10 Fundamentals of high frequency currents   121
2.01 to 2.10 Fundamentals of high frequency currents   122
Semiconductor Diode
• When an n-type semiconductor, which has
  free electrons, is placed in contact with a p-
  type semiconductor, which has positive holes,
  electron move from the n-type to occupy the
  holes in the p-type, while positive holes move
  in the reverse direction.
• In this device the current can only pass in one
  direction, i.e. from p—>n, and such a device is
  called a semiconductor diode.
           2.01 to 2.10 Fundamentals of high frequency currents   123
2.01 to 2.10 Fundamentals of high frequency currents   124
2.01 to 2.10 Fundamentals of high frequency currents   125
2.01 to 2.10 Fundamentals of high frequency currents   126
Construction of The
            Semiconductor Diode
• When the semiconductors n-type and p-type are
  connected to a source of EMF, the PD at their
  junction affects the current flow.
• If the n-type semiconductor is made more
  negative, than the equilibrium value, and the p-
  type more positive, electrons lost from the n-
  type are replaced from the supply, while excess
  electrons are withdrawn from the p-type to the
  supply.
           2.01 to 2.10 Fundamentals of high frequency currents   127
• The PD at the junction is reduced, electrons
  are able to pass from the n-type to the p-type
  and current flows across the circuit.
• If however, the p-type semiconductor is
  negative, relative to the n-type, the PD at the
  junction opposes the electron movement, and
  no current flows until the applied PD reaches
  a certain critical value.

           2.01 to 2.10 Fundamentals of high frequency currents   128
• The current can flow only when ‘n’ is negative
  and ‘p’ is positive, constituting a
  unidirectional flow like a valve, so called as
  semiconductor diode.



          2.01 to 2.10 Fundamentals of high frequency currents   129
Transistor



2.01 to 2.10 Fundamentals of high frequency currents   130
• Transistors are electrical device, which utilize
  a sandwich, of p and n-type semiconductor
  materials.
• It can be NPN, or PNP types.
• In a NPN transistor the two thick layers of n-
  type semiconductors are separated by a thin
  layer of p-type.
• The semiconductor has got three parts:
  Emitter, Base, Collector.
           2.01 to 2.10 Fundamentals of high frequency currents   131
• One of the n-type at the left is the emitter,
  the other at the right is the collector, and the
  central p-type is the base.
• On contact being made between materials,
  say n-p-n semiconductors in this case, PD
  develops at their junctions, the emitter and
  the collector, being positive relative to the
  base.

           2.01 to 2.10 Fundamentals of high frequency currents   132
• When the device is connected to a source of
  EMF, with the emitter negative and the
  collector positive, no current flows unless the
  EMF exceeds the critical value, as the
  electrons are unable to pass from the
  negative p-type to the positive n-type
  semiconductor, so cannot cross the base
  collector junction.

           2.01 to 2.10 Fundamentals of high frequency currents   133
2.01 to 2.10 Fundamentals of high frequency currents   134
2.01 to 2.10 Fundamentals of high frequency currents   135
• A second source of EMF is connected to the
  base and the emitter, the base being positive
  relative to the emitter.
• The electrons can pass from the negative n-
  type to the positive p-type semiconductor.
• So the current flows across the base collector
  junction.

           2.01 to 2.10 Fundamentals of high frequency currents   136
• In the circuit described, there is a thick layer
  of n-type semiconductor, a thin layer of p-
  type semiconductor, so the current consist
  largely of the movement of electrons and the
  electrons from the emitter soon pass into the
  base.



           2.01 to 2.10 Fundamentals of high frequency currents   137
• The base has now an adequate supply of
  electrons, and as it is very thin these come
  close to the base collector junction, and are
  attracted into the collector, to replace those
  that had migrated into the base.
• This reduces the barrier effect across the
  base-collector junction, and current flows
  across the transistor.

           2.01 to 2.10 Fundamentals of high frequency currents   138
• Thus a current fed into the base, renders the
  transistor capable of conducting current, and
  small variations in this base current, causes
  greater variation of current flowing across the
  transistor.
• In this respect the current fed into the base of
  the transistor has an effect, comparable to
  that of a positive charge applied to the grid of
  a triode valve.
           2.01 to 2.10 Fundamentals of high frequency currents   139
2.01 to 2.10 Fundamentals of high frequency currents   140
2.01 to 2.10 Fundamentals of high frequency currents   141
2.01 to 2.10 Fundamentals of high frequency currents   142
Uses of Transistor

• Transistors are used in preference to the
  valves, in most modern electrical equipment,
  as they are durable, have a long life, consume
  less power and need no heating device.
• As the power output is limited they are
  suitable for use in the production of low
  frequency but fail to produce high frequency
  currents. e.g. SWD.

          2.01 to 2.10 Fundamentals of high frequency currents   143
Oscillator circuit


 2.01 to 2.10 Fundamentals of high frequency currents   144
• It is also called as the generator or the
  machine circuit.
• The frequency current is generated by this
  circuit, which consists of a capacitance and
  inductance whose dimensions are arranged to
  allow electron oscillation at a precise
  frequency.


          2.01 to 2.10 Fundamentals of high frequency currents   145
• The frequency (F) at which the circuit will
  oscillate depends only on its electrical size,
  which is the product of capacitance (C) and
  inductance (L):

                                       1
                      F=
                                2Π√LC

           2.01 to 2.10 Fundamentals of high frequency currents   146
• The main function is to give an amplified AC,
  that has a high frequency.
• It consists of,
  I.     Main supply
  II.    Triode valve
  III.   Grid leak resistance
  IV.    Oscillator circuit


              2.01 to 2.10 Fundamentals of high frequency currents   147
1. Main supply: It is connected with AC mains
   that gives 220 or 240 volts and frequency of
   50 cycles/second.
2. Transformer: There are two types of
   transformer which are used in the
   construction, such as:


          2.01 to 2.10 Fundamentals of high frequency currents   148
a. Step down transformer: The secondary coil
   of which is connected with the filament of
   the triode valve and produces a potential of
   20 volts, which causes emission of electrons
   from the cathode through thermionic
   emission.
b. Step up transformer: The secondary coil of
   this transformer is connected with the
   oscillator circuit, which in turn is connected
   with the triode valve.
           2.01 to 2.10 Fundamentals of high frequency currents   149
3. Triode valve: This is the thermionic valve,
   which allows electrons to flow in one direction.
• When the current flows through the filament
   electrons are emitted by thermionic emission
   from the cathode.
• The electrons emitted move towards the
   anode provided the grid does not have any
   charge.

           2.01 to 2.10 Fundamentals of high frequency currents   150
• The grid of the triode valve is connected with
  the grid leak resistance.
• The grid of the triode valve acts as a
  regulator to the flow of the current, i.e. when
  positive allows flow of current and when
  negative stops the current flow.


           2.01 to 2.10 Fundamentals of high frequency currents   151
4. Grid leak resistance: It consists of a
   resistance coil connected to the grid of the
   triode valve at one end and the filament of
   the cathode at the other.
5. Oscillator: It consists of a stable condenser
   and an oscillator coil, which gives high
   magnitude, high frequency oscillating
   currents to the resonator circuit.

           2.01 to 2.10 Fundamentals of high frequency currents   152
Reference


1. Electrotherapy Simplified – Nanda

2. Clayton’s Electrotherapy

3. Electrotherapy Evidence-based Practice –
  Sheila Kitchen


          2.01 to 2.10 Fundamentals of high frequency currents   153

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Fundamentals of high frequency currents priyank

  • 1. 2.01 - 2.10 FUNDAMENTALS OF HIGH FREQUENCY CURRENTS TEACHER : Dr. RINKU SHAH (PT) Dr. KAJAL PATEL (PT) VERIFIED BY : Dr. ASHOK CHAUDHARY (PT) VALIDATED BY : Dr. POONGUNDRAN P. (PT)
  • 2. MAGNETISM 2.01 to 2.10 Fundamentals of high frequency currents 2
  • 3. • A magnet is an object which exhibits certain properties. • For example, when free to rotate, it will align itself in the North—South direction. • It also has the power to attract, and produce magnetism in, certain other materials. • So, A piece of substance, which possesses the property of attracting small pieces of iron towards, it is called a magnet. 2.01 to 2.10 Fundamentals of high frequency currents 3
  • 4. • If the property of magnetism occurs naturally the magnet is known as a Natural magnet. • It is possible artificially to induce magnetism by rubbing the given piece of substance with magnets. – The magnet thus produced is called an Artificial Magnet. 2.01 to 2.10 Fundamentals of high frequency currents 4
  • 5. The molecular theory of magnetism • No matter how many times a magnet is divided, it will always present a North and a South pole. • This phenomenon could conceivably be carried on down to molecular level, where it is thought that the revolving electrons produce a North and a South pole for each molecule, giving so-called ‘Molecular Magnets’. 2.01 to 2.10 Fundamentals of high frequency currents 5
  • 6. • In a non-magnetized state, these molecular magnets are arranged in a haphazard way and cancel out one another’s effects. • In the magnetized state, the molecular magnets are ordered so that one end of the piece of metal exhibits a North pole and the other a South. 2.01 to 2.10 Fundamentals of high frequency currents 6
  • 7. • In magnetized materials such as steel, the friction between the molecules is great and the ordered magnetic effect is retained, giving a permanent magnet. • Heating or banging will, however, disrupt the order and so the magnetism will be lost. 2.01 to 2.10 Fundamentals of high frequency currents 7
  • 8. • Haphazard arrangement of molecular magnets. 2.01 to 2.10 Fundamentals of high frequency currents 8
  • 9. • Ordered arrangement of molecular magnets 2.01 to 2.10 Fundamentals of high frequency currents 9
  • 10. • In a material such as soft iron there is little friction between the molecules, so although they can easily be influenced into an ordered pattern, this pattern will also be lost very easily. • Thus soft iron only forms temporary magnets • The magnetic effect of a wire carrying an electric current can be used to create an electromagnet, which exists only for as long as current flows. 2.01 to 2.10 Fundamentals of high frequency currents 10
  • 11. • Magnetization by contact. 2.01 to 2.10 Fundamentals of high frequency currents 11
  • 12. • The magnetic field around a bar magnet. 2.01 to 2.10 Fundamentals of high frequency currents 12
  • 13. Magnetic Poles • The points inside the magnet, where attraction is maximum are called poles. • Every magnet has two poles: north pole and south pole. • A freely suspended magnet sets itself in the direction of geographic north and south. 2.01 to 2.10 Fundamentals of high frequency currents 13
  • 14. • North pole: The end of the magnet pointing towards north is called north seeking pole or north pole. • South pole: The end of the magnet pointing towards south is called south seeking pole or south pole. 2.01 to 2.10 Fundamentals of high frequency currents 14
  • 15. • In a magnet the unlike poles attract each other and like poles repel each other. • Two magnets one of which is suspended comes closer to the other when their opposite poles are kept nearer, whereas it moves apart when their like poles are kept nearer. 2.01 to 2.10 Fundamentals of high frequency currents 15
  • 16. Properties of a magnet 1. Setting in a North—South direction As the Earth itself is a giant magnet, the Earth’s magnetic field will influence a suspended magnet so that one of its poles (ends) will settle in the direction of the Earth’s North Pole. 2.01 to 2.10 Fundamentals of high frequency currents 16
  • 17. 2. Like magnetic poles repel one another North repels North and South repels South. • Unlike magnetic poles attract one another, i.e. North attracts South and South attracts North. 2.01 to 2.10 Fundamentals of high frequency currents 17
  • 18. 3. Transmission of properties: A magnet can produce properties of magnetism in suitable materials. • As one pole of a bar magnet is stroked along the material; all the opposite poles of the molecular magnets are attracted towards it so that the object is magnetized. • The end that the magnet leaves will have the pole opposite to that used to induce the effect. 2.01 to 2.10 Fundamentals of high frequency currents 18
  • 19. • A magnet may also produce a magnetic effect in an object without contact between them (magnetic induction). • Once again, it is the influence of the magnet over the molecular magnets of the susceptible materials which produces the magnetic effect. 2.01 to 2.10 Fundamentals of high frequency currents 19
  • 20. 4. Attraction of suitable materials Magnets attract certain materials. • This effect is produced by magnetic induction. 2.01 to 2.10 Fundamentals of high frequency currents 20
  • 21. 5. A magnetic field: This is the area or zone of influence around a magnet in which its magnetic forces are apparent. 2.01 to 2.10 Fundamentals of high frequency currents 21
  • 22. • This field may be considered as being made up of magnetic lines of force which have the following properties: a) They travel from North to South, which is the path a free North Pole would take. b) They attempt to take the shortest route possible but repel one another so that they in fact become curved. c) They travel more easily through some materials, e.g. metals, than through others. 2.01 to 2.10 Fundamentals of high frequency currents 22
  • 23. Types of Magnet Magnets are of two types • Natural magnets: The magnets found in nature are called natural magnets. These magnets are weak and shapeless. • Artificial magnets: Man made magnets are called artificial mans. These magnets are strong and of different shapes. • They may be bar shaped, horseshoe shaped, magnetic needles, magnetic compass, etc. 2.01 to 2.10 Fundamentals of high frequency currents 23
  • 24. Types of Artificial Magnets 1. Temporary magnets: Magnetism of these magnets is temporary. It is made of soft iron. 2. Permanent magnet: Magnetism of these magnets is permanent. It is made up of steel, nickel and cobalt. 2.01 to 2.10 Fundamentals of high frequency currents 24
  • 25. Electromagnetism 2.01 to 2.10 Fundamentals of high frequency currents 25
  • 26. • Electromagnetism is one of the four fundamental forces known to exist in the universe. • An electromagnet consists of a coil of wire wound onto a soft iron bar. • When a current passes through the wire it magnetizes the bar by induction. 2.01 to 2.10 Fundamentals of high frequency currents 26
  • 27. • As soon as the current is put off, the magnetic effect is lost. • Wires carrying an electric current produce magnetic field around a straight wire in the form of concentric circles with the wire at their center. 2.01 to 2.10 Fundamentals of high frequency currents 27
  • 28. • A coil of wire produces a field somewhat similar to that of a bar magnet, with the main difference being that in electromagnetism a uniform field is produced inside it. • This uniformity of field is used as an advantage in SWD application. 2.01 to 2.10 Fundamentals of high frequency currents 28
  • 29. • A coil of wire produces a field somewhat similar to that of a bar magnet, with the main difference being that in electromagnetism a uniform field is produced inside it. This uniformity of field is used as an advantage in SWD application. 2.01 to 2.10 Fundamentals of high frequency currents 29
  • 30. Electromagnetic induction • Electromagnetic induction is the means by which electricity is produced from magnetism (and vice-versa). • It is the result of interaction between a conductor and magnetic lines of force. • An EMF is produced in the conductor by the magnetic lines of force surrounding a magnet, without contact between the magnet and the conductor. 2.01 to 2.10 Fundamentals of high frequency currents 30
  • 31. Electromagnetic induction • The factors essential to electromagnetic induction are: 1. Conductor 2. Magnetic lines of force 3. Relative movement of 1 and 2 2.01 to 2.10 Fundamentals of high frequency currents 31
  • 32. Electromagnetic induction • If the conductor is part of a closed circuit, the magnetic lines of force produce an EMF which causes movement of the electrons in the conductor. • This can be shown with an ammeter connected across a coil of wire When a magnet is moved into the coil, the magnetic lines of force cut across the conducting wire of the coil and cause movement of electrons in the coil. 2.01 to 2.10 Fundamentals of high frequency currents 32
  • 33. Electromagnetic induction • These electrons repel adjacent electrons and so on, and a current is set up in the circuit. Movement of the ammeter needle, indicating current flow, will be seen only when either the magnet or the coil is moving. If the magnetic lines of force are stationary relative to the coil of wire, there is no induction. 2.01 to 2.10 Fundamentals of high frequency currents 33
  • 34. • Electromagnetic induction also occurs if the magnetic field used is that surrounding a coil Of wire. • The principles are the same. There must be movement of the magnetic field relative to the conductor. 2.01 to 2.10 Fundamentals of high frequency currents 34
  • 35. • This may be achieved by using an alternative current in the primary coil which causes the magnetic field to build up, fall, then build up in the opposite direction, then fall, etc. • The current builds up to a maximum positive value and then falls to zero. It then drops to a maximum negative value before returning to zero. This rise and fall of current produces movement of the magnetic lines of force. 2.01 to 2.10 Fundamentals of high frequency currents 35
  • 36. • In practice, the conductor in which the EMF is induced is usually a coil of wire, while the magnetic field used to induce the EMF is that of a permanent magnet or a current-carrying coil of wire. 2.01 to 2.10 Fundamentals of high frequency currents 36
  • 37. • Movement of one of these relative to the other is achieved either by spinning the conductor in the magnetic field, as in a dynamo, or by varying the intensity of current in the coil of wire, as in a transformer 2.01 to 2.10 Fundamentals of high frequency currents 37
  • 38. The direction of the induced EMF • The direction in which the magnetic lines of force move relative to the conductor affects the direction in which the induced current flows. This can again be seen by using the bar magnet and coil. 2.01 to 2.10 Fundamentals of high frequency currents 38
  • 39. The direction of the induced EMF • As the magnet is moved into the coil, the ammeter needle deflected in one direction. • As it is withdrawn, deflection occurs in the opposite direction, thus demonstrating that the direction of current flow changes with a reversal of movement of the magnetic field. 2.01 to 2.10 Fundamentals of high frequency currents 39
  • 40. The direction of the induced EMF • The same is true when the inducing magnetic field is that surrounding a current-carrying coil of wire. • As the current rises and the magnetic lines of force move out, thus cutting the conductor, deflection of the ammeter needle occurs in one direction. 2.01 to 2.10 Fundamentals of high frequency currents 40
  • 41. The direction of the induced EMF • As the current drops to zero, the magnetic lines of force move back in towards the primary coil. The direction of movement of these lines of force is now reversed, and so is the direction of the induced current indicated by the ammeter. 2.01 to 2.10 Fundamentals of high frequency currents 41
  • 42. The direction of the induced EMF • This result is often quoted as Lenz’s law, which states that the direction of the induced EMF is such that it tends to oppose the force producing it. 2.01 to 2.10 Fundamentals of high frequency currents 42
  • 43. The strength of the induced EMF • This depends upon two factors: 1. the rate of change of the magnetic field 2. the inductance of the conductor 2.01 to 2.10 Fundamentals of high frequency currents 43
  • 44. 1 The rate of change of the magnetic field • The more rapid the movement of the permanent magnet and the stronger the magnet used, the greater is the rate at which the magnetic lines of force cut the conductor and the greater the induced EMF. 2.01 to 2.10 Fundamentals of high frequency currents 44
  • 45. 1 The rate of change of the magnetic field • In the case of a current-carrying coil of wire, if the frequency of current is increased (and hence the rate of rise and collapse of the magnetic field), a stronger EMF is induced. 2.01 to 2.10 Fundamentals of high frequency currents 45
  • 46. 2 The inductance of the conductor • Inductance is the ability of a conductor to have a current induced in it. Inductance is measured in henries. • Inductance is constant for any particular conductor, but high inductance can be designed into a conducting coil by incorporating the following principles: 2.01 to 2.10 Fundamentals of high frequency currents 46
  • 47. 2 The inductance of the conductor 1. Using many turns of wire in the coil 2. Placing the turns close together 3. Winding the coil onto a soft iron core • This ensures that the magnetic lines of force cut the maximum number of coils in the conductor and thus induce a strong EMF into it. 2.01 to 2.10 Fundamentals of high frequency currents 47
  • 48. LAWS 2.01 to 2.10 Fundamentals of high frequency currents 48
  • 49. Faraday’s Law of Electromagnetic Induction • Faraday’s laws deal with the induction of EMF in an electrical circuit, when magnetic flux linked with the circuit changes. 2.01 to 2.10 Fundamentals of high frequency currents 49
  • 50. Faraday’s Law of Electromagnetic Induction • Whenever magnetic flux linked with a circuit changes, an EMF is induced in it. • An induced EMF exists in the circuit, so long as the change in magnetic flux linked with it continues. • The induced EMF is directly proportional to the negative rate of change of magnetic flux linked with the circuit. 2.01 to 2.10 Fundamentals of high frequency currents 50
  • 51. Lenz’s Law • The law states that the direction of the induced EMF (current) is such that it opposes the very cause, which produces it. 2.01 to 2.10 Fundamentals of high frequency currents 51
  • 52. Fleming’s Right Hand Rule • It gives us the direction of the induced EMF (current), in a conductor moving in a magnetic field. It states that, if the thumb, index and middle fingers of the right hand are stretched mutually perpendicular, then thumb indicates motion, index finger indicates the direction of the field and middle finger indicates the direction of induced current. 2.01 to 2.10 Fundamentals of high frequency currents 52
  • 53. Mutual Induction • Mutual induction is said to occur when an EMF is induced in an adjacent conductor by the magnetic field set-up around a coil of wire carrying a varying current. In a transformer and in physiotherapy this principle is very much used in the electrotherapeutic modalities, e.g. SWD. 2.01 to 2.10 Fundamentals of high frequency currents 53
  • 54. Self Induction • Self induction occurs with in a coil carrying a varying current. A magnetic field is set-up around each turn of wire. • As the current increases, the magnetic lines of force move out, cutting adjacent turns of wire and thus inducing an EMF in them. 2.01 to 2.10 Fundamentals of high frequency currents 54
  • 55. Self Induction • Following Lenz’s law, the direction of the induced EMF will be opposite to the force (or current) producing it. • Therefore, the induced EMF is in the opposite direction to the main current and so opposes its rise. Self induced EMF of this type is therefore, called back EMF. 2.01 to 2.10 Fundamentals of high frequency currents 55
  • 56. Self Induction • A similar sequence of events occurs when the primary current starts to fall. The magnetic field now collapses and the lines of force move back in, cutting adjacent turns of wire but in the opposite direction from before. • Consequently, the induced EMF is also in the opposite direction and flows forward as the forward EMF. 2.01 to 2.10 Fundamentals of high frequency currents 56
  • 57. Self Induction • The overall effect of back and forward EMF is to retard the rate of rise of current and prolong its fall. 2.01 to 2.10 Fundamentals of high frequency currents 57
  • 58. Choke coil • It is a device included in the circuit to produce self induced EMF, maintaining a smooth flow of current. It is of two types, i.e. low frequency choke coil and high frequency choke coil. 2.01 to 2.10 Fundamentals of high frequency currents 58
  • 59. Low Frequency Choke Coil Choke coil • This consists of many turns of insulated wire, wound on a laminated soft iron frame, usually on the central bar of a rectangular frame 2.01 to 2.10 Fundamentals of high frequency currents 59
  • 60. Low Frequency Choke Coil Choke coil • When a current, which varies in intensity, is passed through the coil, magnetic lines of force are set-up, which cut the turns of wire and induce EMF in them. • There are many turns of wire, so the coil has considerable inductance and self-induced EMF is large. 2.01 to 2.10 Fundamentals of high frequency currents 60
  • 61. Low Frequency Choke Coil Choke coil • The core serves to concentrate the magnetic field, it is made of soft iron, so that it is easily magnetized and de-magnetized, and is laminated to prevent eddy currents. 2.01 to 2.10 Fundamentals of high frequency currents 61
  • 62. High Frequency Choke Coil • A high frequency current varies very rapidly in intensity so tend to produce a considerable self-induced EMF. • Consequently, it is unnecessary to have many turns of wire, in a high frequency choke coil, or to wind them on a soft iron core. • The coil usually consists of several turns of insulated wire wound on the bobbin of some non-conducting material. 2.01 to 2.10 Fundamentals of high frequency currents 62
  • 63. Uses of choke coil • To even out the variations in the intensity of the current, providing a smooth current flow: The self-induced EMF, which is set-up when a varying current is passed through a choke coil, retards the rise of current to a maximum, and prolongs the current flow, when the intensity is falling, there by maintaining an even flow of current. 2.01 to 2.10 Fundamentals of high frequency currents 63
  • 64. Uses of choke coil • To prevent the flow of a high frequency current and allow the passage of the low frequency one: When a high frequency current is passed through a choke coil, the inductive reactance is considerable, there by retarding the flow of such a current, 2.01 to 2.10 Fundamentals of high frequency currents 64
  • 65. Uses of choke coil when a low frequency current is passed, the impedance to current flow is very less, due to which the choke coil serves the above function. 2.01 to 2.10 Fundamentals of high frequency currents 65
  • 66. Eddy Current • Any conductor lying in a varying magnetic field has an EMF induced in it. If the conductor is solid, the magnetic lines of force passing through it set-up circular currents called eddy currents 2.01 to 2.10 Fundamentals of high frequency currents 66
  • 67. Eddy Current • In the figure shown below, the solid conductor ‘B’ is present in the varying magnetic field which produces the eddy currents in it shown by the arrow pointing up and down. 2.01 to 2.10 Fundamentals of high frequency currents 67
  • 68. Eddy Current • These eddy currents are perpendicular to the magnetic lines of force and produce heating effect in tissues in accordance with Joules 2.01 to 2.10 Fundamentals of high frequency currents 68
  • 69. Transformer 2.01 to 2.10 Fundamentals of high frequency currents 69
  • 70. • It is a device used for changing low alternating voltage at high current. It changes the alternating voltage without the loss of energy. 2.01 to 2.10 Fundamentals of high frequency currents 70
  • 71. Types of Transformer • Broadly the transformers are divided into three types 1. static transformer 2. variable transformer 3. autotransformer 2.01 to 2.10 Fundamentals of high frequency currents 71
  • 72. Static Transformer • The static transformer is based on the principles of electromagnetic induction, and is used to alter voltage of an alternating current and to render the current earth free. 2.01 to 2.10 Fundamentals of high frequency currents 72
  • 73. Static Transformer- construction • It consists of two coils of insulated wire, the primary and the secondary coils, wound on a laminated soft iron core. 2.01 to 2.10 Fundamentals of high frequency currents 73
  • 74. Static Transformer- construction • The coils are completely insulated from each other and one usually contains more turns of wire than the other. • The frame is often rectangular in shape and the coils may be wound on opposite bars of the frame or one on top of the other on a central bar. 2.01 to 2.10 Fundamentals of high frequency currents 74
  • 75. Static Transformer- working • An alternating current is passed through the primary coil and sets up a varying magnetic field, which cuts the secondary coil and induces an EMF in it. • It is essential that the primary current varies in intensity, otherwise there is no movement of the magnetic field relative to the conductor and no EMF is induced in the secondary coil. 2.01 to 2.10 Fundamentals of high frequency currents 75
  • 76. Static Transformer- working • There is no electrical conduction between the primary and the secondary coils, the energy being transmitted from one to the other by electromagnetic induction. • The core serves to concentrate the magnetic field and is made of soft iron, as this material is easily magnetized and de magnetized. It is laminated to prevent eddy currents. 2.01 to 2.10 Fundamentals of high frequency currents 76
  • 77. Static Transformer- functions 1. Alters the voltage of an alternating current • The EMF induced in the secondary coil depends upon the number of turns of wire it has, relative to the primary coil. Depending on this number of turns, the transformers can be classified as: – Step up transformer – Step down transformer – Even ration transformer 2.01 to 2.10 Fundamentals of high frequency currents 77
  • 78. Step up transformer • If the number of turns in the secondary are more than that of the primary, the voltage developed in the secondary will be increased or stepped up. Such a device is called as step up transformer. 2.01 to 2.10 Fundamentals of high frequency currents 78
  • 79. Step down transformer • If the secondary coil has fewer turns than the primary, then the EMF, or voltage in the secondary will be less than in the primary, i.e. it is stepped down. Such an arrangement produces a step down transformer. 2.01 to 2.10 Fundamentals of high frequency currents 79
  • 80. Even ratio transformer • If the number of turns in the primary and secondary coils are same, the voltage in the primary is same as that of the secondary. Such a device is called even ratio transformer. • It is important to note that, the electrical power in both the primary and the secondary circuits are always the same. 2.01 to 2.10 Fundamentals of high frequency currents 80
  • 81. Even ratio transformer • Power is measured in watts (volts x ampere), so the quantity watts x ampere must be same for both the primary and secondary coils, i.e. any change in voltage must be accompanied by a change in current. 2.01 to 2.10 Fundamentals of high frequency currents 81
  • 82. Static Transformer- functions 2. Renders a current earth free • The mains electricity is produced by the dynamo, and the consumer is supplied with a wire at high potential, called the live wire, and a wire at zero potential connected to earth, called the neutral wire. 2.01 to 2.10 Fundamentals of high frequency currents 82
  • 83. • Most electrical apparatus works on a current, which flows from the live wire, through the apparatus, to the neutral wire and earth. 2.01 to 2.10 Fundamentals of high frequency currents 83
  • 84. • If an accidental connection is made between live wire and earth, current will flow along it. • If this connection were made through a person, they would then receive an earth shock, as the current flows through them to earth. 2.01 to 2.10 Fundamentals of high frequency currents 84
  • 85. • The static transformer reduces this danger by using electromagnetic induction, to transfer the electrical energy into the secondary coil where earth plays no part in the circuit. 2.01 to 2.10 Fundamentals of high frequency currents 85
  • 86. • The effect on the secondary coil of the magnetic field around the primary is to cause electrons to move around the secondary circuit, but not to leave it. Earth plays no part in the secondary circuit, because, even if an earth connection is made with it, electrons will not leave the circuit, but will continue to flow around it 2.01 to 2.10 Fundamentals of high frequency currents 86
  • 87. • This is an important safety factor, and that all currents applied to patients are rendered earth free by using a static transformer. 2.01 to 2.10 Fundamentals of high frequency currents 87
  • 88. Variable Transformer • It consists of a primary and secondary coil, but is constructed so that one of them can be altered in length. 2.01 to 2.10 Fundamentals of high frequency currents 88
  • 89. Variable Transformer • The primary coil has a number of tapings taken from it and a movable contact can be made on any one of these by turning a knob. • The effect of decreasing the number of turns in the primary coil relative to the secondary is to cause a step up voltage in the secondary coil. In his way a very crude control of voltage is obtained. 2.01 to 2.10 Fundamentals of high frequency currents 89
  • 90. Autotransformer • It consists of a single coil of wire with four contact points coming from it. 2.01 to 2.10 Fundamentals of high frequency currents 90
  • 91. Autotransformer • It can be used as a step up, or a step down transformer. When used as the step up, CD is the primary coil and AB is the secondary coil. When used as the step down, AB is the primary and CD is the secondary coil. Although the autotransformer works on the 2.01 to 2.10 Fundamentals of high frequency currents 91
  • 92. Autotransformer • Although the autotransformer works on the principles of electromagnetic inductions, it has the disadvantage that, it allows only a small step up, and does not render the current earth free. • It is used in the starter circuit of ultraviolet lamp to strike the arc in the lamp. 2.01 to 2.10 Fundamentals of high frequency currents 92
  • 93. Diode & triode valves 2.01 to 2.10 Fundamentals of high frequency currents 93
  • 94. Valve • Valve is a device, which transmits the flow in one direction only, common examples being that of the valves of heart, or vein. • In electronics a thermionic valve is defined as a device allowing unidirectional flow of current. 2.01 to 2.10 Fundamentals of high frequency currents 94
  • 95. Valve • There are various types of thermionic valves, which are named according to the number of electrodes they contain. They are: 1. Diode valve 2. Triode valve 2.01 to 2.10 Fundamentals of high frequency currents 95
  • 96. Diode valve • This is the simplest form of thermionic valve, containing a cathode with a filament and an anode, enclosed in an evacuated glass tube. • The valve may either be evacuated or may contain an inert gas at low pressure. 2.01 to 2.10 Fundamentals of high frequency currents 96
  • 97. Diode valve • For the current to pass through the valve, the filament must be heated, causing emission of electrons by the process of thermionic emission & a PD when applied makes the plate (anode) positive in relation to the cathode. 2.01 to 2.10 Fundamentals of high frequency currents 97
  • 98. Diode valve • The filament used can be directly or indirectly heating type and the anode plate is made from some metal, which does not allow thermionic emission readily and is in the form of a cylinder surrounding the cathode. 2.01 to 2.10 Fundamentals of high frequency currents 98
  • 99. Diode valve • The directly heating filament is a loop of fine wire of thoriated tungsten (tungsten can tolerate repeated and cooling, allowing emission of electrons at low temperature) • The indirectly heating filament is a fine loop of wire embedded in some insulated material and the whole device is surrounded by a metal cylinder from which thermionic emission takes place. 2.01 to 2.10 Fundamentals of high frequency currents 99
  • 100. Diode valve • The electrons so emitted will be attracted by the positive anode constituting an electrical current across the device. • When the applied PD is reversed, so that the plate (anode) is negative with respect to the cathode, no current flows through the device, indicating that the electrons can pass from cathode to plate, not in the reverse direction, i.e. the current can flow only in one direction. 2.01 to 2.10 Fundamentals of high frequency currents 100
  • 101. Diode valve • The intensity of current that flows across the valve depends on the heating of the filament and on the PD between the filament and the plate. • If more current is applied to the filament causing increased heating of the same, it will emit more number of electrons and this when combined with an increase in PD, makes available greater force to attract the electrons. 2.01 to 2.10 Fundamentals of high frequency currents 101
  • 102. Diode valve • And there by increasing the current flow across the valve. In a diode there are the filament circuit and the anode circuit. • The diode is symbolically represented and three dimensionally as in Figure 2.01 to 2.10 Fundamentals of high frequency currents 102
  • 103. Triode valve • The triode valve is a device that contains three electrodes viz. cathode, grid, and the anode. • The grid, whose potential can be altered, is placed between the cathode and the anode. • The grid, which surrounds the filament, may consist of a metal cylinder, perforated to allow the electrons to pass through, or may be a spiral of metal wire. 2.01 to 2.10 Fundamentals of high frequency currents 103
  • 104. Triode valve • A lead from the grid is brought to a pin outside the base of the valve, necessitating four pins, i.e. two for the filaments, one for the grid and one for the anode. • When the filament will be heated as like the diode, current passes from the valve in one direction only, i.e. from plate to cathode. 2.01 to 2.10 Fundamentals of high frequency currents 104
  • 105. Triode valve • If the grid is uncharged, it has no effect on the current flow. • If the grid is given with a negative charge from the outside source, it repels electrons, either causing a reduction of current flow, or resulting in complete cessation of current flow. • If however, the grid is given a positive charge, the electrons can pass and the current flows. 2.01 to 2.10 Fundamentals of high frequency currents 105
  • 106. Triode valve • The charges applied to the grid from the external source are called as grid bias. • As the grid lies close to the cathode, than the anode, the charges on the grid has a greater influence, on the flow of current than a similar charge on the anode. • The flow of current across the triode valve can be regulated by adjusting the bias of the grid. 2.01 to 2.10 Fundamentals of high frequency currents 106
  • 107. Triode valve • The triode valve is represented symbolically and three dimensionally as in Figure 2.01 to 2.10 Fundamentals of high frequency currents 107
  • 108. Uses of a triode valve • Used for the production of interrupted current and other muscle stimulating currents. • Used for the production of high frequency currents in conjunction with a condenser and inductance. • It is not used as a rectifier, but rectifies the current that passes through it. • It is used as a switch. 2.01 to 2.10 Fundamentals of high frequency currents 108
  • 109. Semiconductors 2.01 to 2.10 Fundamentals of high frequency currents 109
  • 110. • Semiconductors are usually metals, which because of thermal agitations, or addition of impurities, have electrons free to conduct current. • A semiconductor can either be of n-type, or p- type. 2.01 to 2.10 Fundamentals of high frequency currents 110
  • 111. • In a n-type semiconductor, there is an excess of electron, which carries current, where as in a p-type, the deficiency of electron give rise to positive hole, due to which current flow occurs. • If a n-type and a p-type semiconductors are fused together, electrons can only pass in the n—>p direction, and the semiconductor therefore acts as a valve. 2.01 to 2.10 Fundamentals of high frequency currents 111
  • 112. N-type, Semiconductor • An atom of silicon with atomic number 14, has 4 electrons in the outer shell, and in a crystal of silicon these are held in forming bonds with neighboring atoms, so that there are no free electrons to transmit an electric current. • When certain other materials such as phosphorous (atomic number 15, with 5 electrons outside) are added to silicon it transmits current. 2.01 to 2.10 Fundamentals of high frequency currents 112
  • 113. 2.01 to 2.10 Fundamentals of high frequency currents 113
  • 114. • When silicon and phosphorous form covalent bonds, four electrons of phosphorus make bond with four electrons of silicon, leaving behind one free electron in the phosphorous which are not held in bond with other atoms, therefore carrying current, when connected with a source in the same way like the conductors. • Such a material is called n-type semiconductor. 2.01 to 2.10 Fundamentals of high frequency currents 114
  • 115. 2.01 to 2.10 Fundamentals of high frequency currents 115
  • 116. 2.01 to 2.10 Fundamentals of high frequency currents 116
  • 117. P-type Semiconductor • When silicon is added with certain other substances such as aluminium with an atomic number 13, the three outer electrons in the aluminium atom, makes bond with three electrons in the outer orbit of silicon, whereas for the 4th electron of silicon, there is no electron available on the outer orbit of aluminium, creating an electron deficiency called hole. 2.01 to 2.10 Fundamentals of high frequency currents 117
  • 118. • When a PD is applied to such a material, electrons move from some of the atoms into these unoccupied bonds or holes nearer to the positive poles, so that as the electrons move away from the negative towards the positive, the holes move from the positive towards the negative, constituting a flow of current. 2.01 to 2.10 Fundamentals of high frequency currents 118
  • 119. • The movement of positive holes from positive towards negative is equivalent to the movement of electrons from negative to positive. • The material that transmits current in this manner is called a p-type semiconductor. 2.01 to 2.10 Fundamentals of high frequency currents 119
  • 120. 2.01 to 2.10 Fundamentals of high frequency currents 120
  • 121. 2.01 to 2.10 Fundamentals of high frequency currents 121
  • 122. 2.01 to 2.10 Fundamentals of high frequency currents 122
  • 123. Semiconductor Diode • When an n-type semiconductor, which has free electrons, is placed in contact with a p- type semiconductor, which has positive holes, electron move from the n-type to occupy the holes in the p-type, while positive holes move in the reverse direction. • In this device the current can only pass in one direction, i.e. from p—>n, and such a device is called a semiconductor diode. 2.01 to 2.10 Fundamentals of high frequency currents 123
  • 124. 2.01 to 2.10 Fundamentals of high frequency currents 124
  • 125. 2.01 to 2.10 Fundamentals of high frequency currents 125
  • 126. 2.01 to 2.10 Fundamentals of high frequency currents 126
  • 127. Construction of The Semiconductor Diode • When the semiconductors n-type and p-type are connected to a source of EMF, the PD at their junction affects the current flow. • If the n-type semiconductor is made more negative, than the equilibrium value, and the p- type more positive, electrons lost from the n- type are replaced from the supply, while excess electrons are withdrawn from the p-type to the supply. 2.01 to 2.10 Fundamentals of high frequency currents 127
  • 128. • The PD at the junction is reduced, electrons are able to pass from the n-type to the p-type and current flows across the circuit. • If however, the p-type semiconductor is negative, relative to the n-type, the PD at the junction opposes the electron movement, and no current flows until the applied PD reaches a certain critical value. 2.01 to 2.10 Fundamentals of high frequency currents 128
  • 129. • The current can flow only when ‘n’ is negative and ‘p’ is positive, constituting a unidirectional flow like a valve, so called as semiconductor diode. 2.01 to 2.10 Fundamentals of high frequency currents 129
  • 130. Transistor 2.01 to 2.10 Fundamentals of high frequency currents 130
  • 131. • Transistors are electrical device, which utilize a sandwich, of p and n-type semiconductor materials. • It can be NPN, or PNP types. • In a NPN transistor the two thick layers of n- type semiconductors are separated by a thin layer of p-type. • The semiconductor has got three parts: Emitter, Base, Collector. 2.01 to 2.10 Fundamentals of high frequency currents 131
  • 132. • One of the n-type at the left is the emitter, the other at the right is the collector, and the central p-type is the base. • On contact being made between materials, say n-p-n semiconductors in this case, PD develops at their junctions, the emitter and the collector, being positive relative to the base. 2.01 to 2.10 Fundamentals of high frequency currents 132
  • 133. • When the device is connected to a source of EMF, with the emitter negative and the collector positive, no current flows unless the EMF exceeds the critical value, as the electrons are unable to pass from the negative p-type to the positive n-type semiconductor, so cannot cross the base collector junction. 2.01 to 2.10 Fundamentals of high frequency currents 133
  • 134. 2.01 to 2.10 Fundamentals of high frequency currents 134
  • 135. 2.01 to 2.10 Fundamentals of high frequency currents 135
  • 136. • A second source of EMF is connected to the base and the emitter, the base being positive relative to the emitter. • The electrons can pass from the negative n- type to the positive p-type semiconductor. • So the current flows across the base collector junction. 2.01 to 2.10 Fundamentals of high frequency currents 136
  • 137. • In the circuit described, there is a thick layer of n-type semiconductor, a thin layer of p- type semiconductor, so the current consist largely of the movement of electrons and the electrons from the emitter soon pass into the base. 2.01 to 2.10 Fundamentals of high frequency currents 137
  • 138. • The base has now an adequate supply of electrons, and as it is very thin these come close to the base collector junction, and are attracted into the collector, to replace those that had migrated into the base. • This reduces the barrier effect across the base-collector junction, and current flows across the transistor. 2.01 to 2.10 Fundamentals of high frequency currents 138
  • 139. • Thus a current fed into the base, renders the transistor capable of conducting current, and small variations in this base current, causes greater variation of current flowing across the transistor. • In this respect the current fed into the base of the transistor has an effect, comparable to that of a positive charge applied to the grid of a triode valve. 2.01 to 2.10 Fundamentals of high frequency currents 139
  • 140. 2.01 to 2.10 Fundamentals of high frequency currents 140
  • 141. 2.01 to 2.10 Fundamentals of high frequency currents 141
  • 142. 2.01 to 2.10 Fundamentals of high frequency currents 142
  • 143. Uses of Transistor • Transistors are used in preference to the valves, in most modern electrical equipment, as they are durable, have a long life, consume less power and need no heating device. • As the power output is limited they are suitable for use in the production of low frequency but fail to produce high frequency currents. e.g. SWD. 2.01 to 2.10 Fundamentals of high frequency currents 143
  • 144. Oscillator circuit 2.01 to 2.10 Fundamentals of high frequency currents 144
  • 145. • It is also called as the generator or the machine circuit. • The frequency current is generated by this circuit, which consists of a capacitance and inductance whose dimensions are arranged to allow electron oscillation at a precise frequency. 2.01 to 2.10 Fundamentals of high frequency currents 145
  • 146. • The frequency (F) at which the circuit will oscillate depends only on its electrical size, which is the product of capacitance (C) and inductance (L): 1 F= 2Π√LC 2.01 to 2.10 Fundamentals of high frequency currents 146
  • 147. • The main function is to give an amplified AC, that has a high frequency. • It consists of, I. Main supply II. Triode valve III. Grid leak resistance IV. Oscillator circuit 2.01 to 2.10 Fundamentals of high frequency currents 147
  • 148. 1. Main supply: It is connected with AC mains that gives 220 or 240 volts and frequency of 50 cycles/second. 2. Transformer: There are two types of transformer which are used in the construction, such as: 2.01 to 2.10 Fundamentals of high frequency currents 148
  • 149. a. Step down transformer: The secondary coil of which is connected with the filament of the triode valve and produces a potential of 20 volts, which causes emission of electrons from the cathode through thermionic emission. b. Step up transformer: The secondary coil of this transformer is connected with the oscillator circuit, which in turn is connected with the triode valve. 2.01 to 2.10 Fundamentals of high frequency currents 149
  • 150. 3. Triode valve: This is the thermionic valve, which allows electrons to flow in one direction. • When the current flows through the filament electrons are emitted by thermionic emission from the cathode. • The electrons emitted move towards the anode provided the grid does not have any charge. 2.01 to 2.10 Fundamentals of high frequency currents 150
  • 151. • The grid of the triode valve is connected with the grid leak resistance. • The grid of the triode valve acts as a regulator to the flow of the current, i.e. when positive allows flow of current and when negative stops the current flow. 2.01 to 2.10 Fundamentals of high frequency currents 151
  • 152. 4. Grid leak resistance: It consists of a resistance coil connected to the grid of the triode valve at one end and the filament of the cathode at the other. 5. Oscillator: It consists of a stable condenser and an oscillator coil, which gives high magnitude, high frequency oscillating currents to the resonator circuit. 2.01 to 2.10 Fundamentals of high frequency currents 152
  • 153. Reference 1. Electrotherapy Simplified – Nanda 2. Clayton’s Electrotherapy 3. Electrotherapy Evidence-based Practice – Sheila Kitchen 2.01 to 2.10 Fundamentals of high frequency currents 153