Chelmsford Amateur Radio Society Advanced Course (3) Technical Aspects Part-2 - Resistors and Capacitors - PowerPoint PPT Presentation

About This Presentation
Title:

Chelmsford Amateur Radio Society Advanced Course (3) Technical Aspects Part-2 - Resistors and Capacitors

Description:

Chelmsford Amateur Radio Society Advanced Course (3) Technical Aspects Part-2 - Resistors and Capacitors Voltage Drop Source Resistance ElectroMotive Force - EMF ... – PowerPoint PPT presentation

Number of Views:142
Avg rating:3.0/5.0
Slides: 18
Provided by: CarlG76
Category:

less

Transcript and Presenter's Notes

Title: Chelmsford Amateur Radio Society Advanced Course (3) Technical Aspects Part-2 - Resistors and Capacitors


1
Chelmsford Amateur Radio Society Advanced
Course(3) Technical AspectsPart-2 - Resistors
and Capacitors
2
Voltage Drop
  • In any closed circuit if current is flowing there
    must be a voltage drop across circuit elements.
  • This follows OHMS LAW which is recalled as-
  • R V / I V I . R I V /R

3
Source Resistance
  • There is NO ideal source.
  • Every source has some internal resistance.
  • This is termed Source Resistance/Impedance.
  • When current is drawn there is a voltage drop
    across this internal resistance/impedance
  • Source resistance limits the amount of power that
    can be drawn.
  • Example Lead Acid cells have very low internal
    resistance

4
ElectroMotive Force - EMF
  • EMF is the unloaded potential difference between
    two points.
  • The electromotive force of a source is that force
    which tends to cause a movement of electricity in
    a circuit.
  • It has an unloaded voltage V which can be
    transposed to the output terminals provided no
    current flows.

5
Potential Difference
  • The loaded voltage is the Potential Difference
    between two points when current is flowing in the
    circuit.
  • There is now a potential difference across the
    load as current is flowing. The value of which
    follows Ohm's Law.

6
Resistors in Series/Parallel
  • Resistors in Series-
  • Rtotal R1 R2 R3 . . .
  • Resistors in Parallel-
  • 1/Rtotal 1/R11/R21/R3 . . .

7
DC Power
  • Power is measured in WATTS.
  • The calculation for power in a circuit is Volts
    multiplied by Amps
  • P V . I
  • and also
  • P I2 x R P V2 / Rfrom using Ohms Law for V
    or I

8
Potential Dividers
  • By connecting resistors in series a potential
    divider network can be constructed. This is the
    basis of Volume controls, trimmers etc
  • VOUT can be calculated by proportion without
    worrying about the current through the resistors
    if load is high impedance at VOUT.
  • VOUT VIN x R2 / ( R1 R2 )

9
Safety Leakage Paths
  • Capacitors can hold a lethal charge when open
    circuit.
  • A parallel resistor can provide a safety leakage
    path to discharge large value capacitors.
  • High value resistors provide a very low current
    drain across a capacitor. For example it can make
    a PSU safer without affecting operation.
  • In a circuit this is known as a BLEED RESISTOR.

10
Capacitance
  • Potential difference between A B. Charge is set
    in motion therefore current flows.
  • The amount of current is determined by the nature
    of the conductor - its Resistance
  • Also a potential difference between A B, but
    other than the short time at switch-on NO current
    will flow.
  • However the negative plate will contain an excess
    of electrons and the positive plate a deficit.
  • The plates are said to be charged and the name
    given to the ability to store charge is
    Capacitance.

11
Capacitors
  • Instead of two ends of wire a capacitor is made
    up of two or more flat parallel plates. The
    capacitance can be calculated.
  • The plates have area "A" and are separated by
    distance "d".
  • The space between the plates is filled with an
    insulating material known as the DIELECTRIC
  • Dielectric can be any insulator - typically
    Oxides, Plastics, or Ceramic

12
Capacitance Charge
  • The Unit of Capacitance is the FARAD after
    Faraday
  • A capacitance of 1 FARAD is when 1 Coulomb of
    charge is stored with 1 Volt PD.
  • Q C.V
  • or
  • Q / C V
  • or
  • Q / V C
  • One Farad is rather large so uF, nF, pF are more
    common

13
Capacitors
  • CAPACITANCE, C is
  • Proportional to the plate area "A".
  • Inversely proportional to the distance between
    the plates "d
  • Depends upon the material used for the
    dielectric.
  • This can be written as C e0 er A / d where
  • C is in Farads
  • A is area of each plate in square metres
  • d is distance between plates in metres.
  • e0 - A constant known as the permittivity of free
    space or vacuum, dry air having a value of
    8.854 x 10-12 .
  • er - or k Relative permittivity of the
    dielectric, chosen for its TEMPERATURE
    STABILITY, BREAKDOWN VOLTAGE

14
Capacitance Formula Dielectric Materials
The formula C e0 er A / d is also written
as C K . A / d where K e0 er
  • The dielectric type in a capacitor will depend
    upon the function the capacitor is to perform in
    a circuit.
  • As frequency increases dielectric loss increases,
  • Each dielectric also has different breakdown
    voltages.
  • Each material will suffer a change in properties
    due to temperature, this will affect the
    capacity.
  • Typical er - Air1, PTFE2, Mica5, ceramics
    10, Hi-k ceramics 10000

15
Capacitors in Parallel
  • Capacitors connected in parallel all have the
    same voltage
  • The charge on them is dependent upon the
    capacitor value.

Ctotal C1 C2 C3
16
Capacitors in Series
  • When capacitors are in series the charge is the
    same in all of the circuit
  • The voltage is divided between capacitors.

1/Ctotal 1/C1 1/C2 1/C3
17
Charge Discharge of a Capacitor
Time C.R Secs. Where C FaradsR Ohms
Write a Comment
User Comments (0)
About PowerShow.com