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Basic Electronics

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Basic Electronics Ia = +3A Ib = -2A Ic = -1A Ia + Ib + Ic = 0 Battery Capacitor circuit Capacitors Capacitors consists of plates separated by an insulating layer. – PowerPoint PPT presentation

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Title: Basic Electronics


1
Basic Electronics
2
Need to know
  • Definition of basic electrical paramater
  • A set of rules for elementary circuit analysis
  • The means of current flow in circuits with
    capacitance

3
Electrical Parameters
  • Potential Difference (V or E)

4
Charges
  • Electrical charges exert an electrostatic force
    on one another.
  • Like charges are repelled from one another.
  • Unlike charges are attracted to one another.

5
Cont.
  • As the distance between two charges increases,
    the force exerted is reduced.

6
cont
  • Work is done when two charges that were initially
    separated are brought together.
  • Negative work is done if the polarities are
    opposite
  • Positive work is done if the polarities are the
    same

7
  • The greater the values of the charges and the
    greater their initial separation the greater will
    be the work that is done.
  • Work ?r0f(r)dr, where
  • f is electrostatic force
  • r is the initial distance between the two charge.

8
  • Potential difference is a measure of the wok
    done.
  • The potential difference is the work done to move
    a unit of positive charge (1 coulomb) from one
    point to the other.

9
The Volt
  • One volt is the energy required to move one
    coulomb a distance of 1 meter against a force of
    1 newton

10
Current
  • A potential difference exists in a system
    whenever positive and negative charges are
    separated.

11
  • Charge separation may be generated by a chemical
    reaction (Voltas battery) or by diffusion
    between two electrolyte solutions with different
    concentrations across a selectively permeable
    barrier such as a cell plasma membrane.

12
  • To say a membrane is permeable is to say the
    membrane has a whole through which a give ion or
    ions can pass and the two chambers are in contact.

13
  • If a region of charge separation exists within a
    conducting medium, then charges move between
    areas of potential difference

14
  • The direction of these charge movements is
    positive charges are attracted to the the region
    with the more negative potential, and negative
    charges are attracted to the regions of positive
    potential.
  • The movement of charges is current flow.

15
Current Flow
  • Current flow is defined as the movement of
    positive charges per unit time.
  • In metal electrodes current is carried by
    electrons which move the opposite direction of
    current flow.

16
  • In nerve and muscle cells current can be carried
    by positive and negative ions in solution

17
Units of current flow
  • One ampere represents the movement of one
    coulomb per second.

18
Flow
  • From Franklins view one can think of current
    flow in terms of bulk flow of a liguid due to
    hydorstatic pressure, flow of a solute in
    response to a concentration gradient or flow of
    heat in response to a temperature gradient.

19
Ease of flow vs. retardation of flow
  • One can think of the flow being retarded or eased
    dependent on many different physical properties
    of the liquid, of the material the flow is moving
    through or the frictional forces operating on
    the material flowing.

20
  • In so far as electrical flow is characterized
    there are two properties that will be used
  • CONDUCTIVITY OR RESISTIVITY

21
  • It should be intuitively obvious that Resistivity
    and Conductivity are the reciprocal concepts The
    ease of flow conductivity and the retardation of
    flow resistivity or
  • Resistance (Conductance)-1

22
Ohms LAw
  • Ohms law says
  • There is a relationship between the driving
    force and the flow of current they should be
    proportional.
  • The proportionality constant is resistance.

23
  • According to Ohms law current, I, that flows
    through a conductor is directly proportional the
    potential difference imposed on it.

24
  • That is
  • E RI
  • Where E is in volts
  • R is in ohms
  • I is in Amps

25
Ohms law variation
  • If conductance (g) is the reciprocal of
    resistance then it follows
  • E/R I or rewritten, E x g I where
  • E is volts
  • I is in amps
  • g is in semens (was mhos)

26
Conductor
  • The object through which an electric current
    flows is a conductor.
  • As charges move through a conductor some of the
    energy is lost through the conversion to heat.
  • This loss is called entropy

27
Conductivity (s)
  • Each type of material has an intrinsic property
    called conductivity (s)

28
Metallic conductors
  • Metallic conductors have very high conductivities
    current moves easily.
  • Different metals have different abilities to
    faithfully represent the current pulse implied on
    them.

29
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30
Aqueous solutions
  • Aqueous solutions containing high ionized salt
    concentrations have somewhat lower values of s

31
Lipids
  • Lipids have low s and thus they are poor
    conductors but are good insulators.

32
  • In resistance terms,
  • Resistance (r) s (length/area)
  • In conductance terms
  • Conductance (siemens) (Area/length)

33
Capacitance
  • Capacitance is the ability to hold a charge of
    opposite sign positive charges on one side,
    negative charges on the other side.

34
Capacitors
  • Capacitors consists of plates separated by an
    insulating layer.
  • The Leyden jar is a capacitor.
  • The lipid portion of a plasma membrane can act
    like a capacitor.
  • Symbolized as Farads

35
Work done separates charges
36
  • The picture represents two plates of a capacitor.

37
  • One can measure this potential difference by
    determining how much work is required to move a
    positive test charge from the surface of y to
    that of x.

38
  • There is a a net excess of positive charges on
    plate x and an equal number of negative charges
    on plate y, resulting in a potential difference
    between two plates.

39
  • Initially, the test charge is attracted by the
  • negative charges on y and weakly repelled by
    the distant positive charges on x.

40
  • As the test charge is moved to the left across
    the gap the attraction by the negative charges
    on y diminishes, but the repulsion by the
    positive charges on x increases.

41
Capacitance Electrostatic forces
  • The results of the above electrostatic
    interactions is a force that opposes the movement
    of the tests charge from y to x.

42
Electrostatic force
  • The net electrostatic force on the test charge is
    constant everywhere between x and y.

43
Work
  • Work is force times distance or
  • W f x D

44
Farads (F)
  • Capacitance is measured in farads (F)
  • The greater the density of charges on the
    capacitor plates the greater the force acting on
    the test charge, and the greater is the resulting
    potential difference across the capacitor.

45
Capacitance charge and potential difference.
  • A linear relationship exists between the amount
    of charge Q stored on a capacitors plates and the
    potential difference across the plates
  • Q (coulombs) C (farads) x E (volts)

46
Capacitance variables
  • Capacitance of a parallel-plate capacitor is
    determined by the area (A) of the two plates and
    the distance between them.

47
  • Increase in charge density increases the
    potential difference

48
  • Increasing the area (A) of the plates increases
    capacitance because a greater amount of charge
    must be deposited on each side to produce the
    same charge density, which is what determines
    the electrostatic force operating on the test
    charge.

49
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50
  • Increasing the distance (D) between the two
    plates does not change the charge density but
    does increase the work to be done because the
    test charge must move a longer distance.
  • See next slide

51
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52
  • The potential difference across a capacitor is
    determined by the excess of positive charges and
    negative charges on its plates. In order for the
    potential across a capacitor to change, the
    amount of electrical charges stored on the
    conductor must change.

53
  • Given the above rules, to charge a capacitor from
    0 to some higher value, the moment-to-moment
    change in potential difference of a given
    capacitor will be an increasing change of force
    due to and increase change in charge density.

54
Change in potential difference across a capacitor
  • The plotted curve of this change in force will be
    an exponential curve.

55
  • Thus the capacitor will charge in an
    instantaneous manner.
  • We will see latter that resistors in parallel
    with capacitors will respond quite a bit
    differently.

56
  • Symbols
  • Battery
  • Voltage source
  • Resistor
  • Capacitor

57
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60
Current loop through a resistor
61
  • Resistance in series add, while resistances in
    parallel add reciprocally

62
  • An arrow designates direction of current flow
    (net movement of positive charges).
  • Ohms law is
  • I Vg V/R

63
  • The algebraic sum of all currents entering or
    leaving a junction is zero.
  • We arbitrarily define current approaching a
    junction as positive and current leaving a
    junction as negative.

64
Battery and resistor in series
65
Resistors in parallel current has alternative
paths
66
  • Ia 3A
  • Ib -2A
  • Ic -1A
  • Ia Ib Ic 0

67
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68
Battery Capacitor circuit
69
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