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ENGR. VIKRAM KUMAR B.E (ELECTRONICS) M.E (ELECTRONICS SYSTEM ENGG:)

CAPACITOR. ENGR. VIKRAM KUMAR B.E (ELECTRONICS) M.E (ELECTRONICS SYSTEM ENGG:) MUET JAMSHORO. Capacitor. A capacitor is a device for storing charge and electrical potential energy. +. Dielectric. _. Capacitor.

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ENGR. VIKRAM KUMAR B.E (ELECTRONICS) M.E (ELECTRONICS SYSTEM ENGG:)

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  1. CAPACITOR ENGR. VIKRAM KUMAR B.E (ELECTRONICS) M.E (ELECTRONICS SYSTEM ENGG:) MUET JAMSHORO

  2. Capacitor • A capacitor is a device for storing charge and electrical potential energy.

  3. + Dielectric _ Capacitor • All capacitors consists of two metal plates separated by an insulator. The insulator is called dielectric. (e.g. polystyrene, oil or air) • Circuit symbol:

  4. Structure of capacitor • Capacitor = conductor (metal plate) + insulator (dielectric) + conductor (metal plate)

  5. Capacitors • Basic capacitor construction Dielectric material The dielectric material is an insulator therefore no current flows through the capacitor Plate 2 Plate 1

  6. Formation of a Capacitor • Capacitors are formed all of the time in everyday situations: • when a charged thunderstorm cloud induces an opposite charge in the ground below, • when you put your hand near the monitor screen of this computer.

  7. Capacitor Storing a charge between the plates • Electrons on the left plate are attracted toward the positive terminal of the voltage source • This leaves an excess of positively charged holes • The electrons are pushed toward the right plate • Excess electrons leave a negative charge _ + _ + - +

  8. Charged Capacitor • A capacitor is said to be charged when there are more electrons on one conductor plate than on the other. When a capacitor is charged, energy is stored in the dielectric material in the form of an electrostatic field.

  9. Capacitance • Consider any isolated pair of conductors with charge Q Capacitance is defined as Unit : farad (F) Where Q = charge on one conductor V= potential difference between two conductors

  10. Capacitance • The capacitance of a conductor is the charge required to cause unit change in the potential of the conductor. • A one-farad capacitor stores one coulomb of charge when a potential of 1 volt is applied across the terminals of the capacitor. • The smaller the change in potential of the conductor when a certain charge is transferred to it, the more charge it can store before breakdown occurs. • In electronics, the microfarad (μF) and the picofarad (pF) are usually used to measure capacitance.

  11. Capacitance of a Capacitor • Note that Q is not the net charge on the capacitor, which is zero. • Capacitance is a measure of a capacitor's ability to store charge. • The more charge a capacitor can hold at a given potential difference, the larger is the capacitance. • Capacitance is also a measure of the energy storage capability of a capacitor.

  12. Capacitance • Fringing – At the edge of the capacitor plates the flux lines extend outside the common surface area of the plates.

  13. Capacitance • Dielectric – Insulator of the capacitor • The purpose of the dielectric is to create an electric field to oppose the electric field setup by free charges on the parallel plates. • Di for “opposing” and electric for “electric field” • Dipoles – Formed within the insulator of a capacitor when the electrons of the insulating material are unable to leave the parent atom and travel to the positive plate of the capacitor

  14. Capacitance • With different dielectric materials between the same two parallel plates, different amounts of charge will deposit on the plates. • Permittivity – The ratio of the flux density to the electric field intensity in the dielectric. A measure of how easily the dielectric will “permit” the establishment of flux lines within the dielectric. • Relative permittivity – Often called the dielectric constant, it is the ratio of the permittivity of any dielectric to that of a vacuum.

  15. Capacitors • Working voltage – the voltage that can be applied across a capacitor for long periods of time with out breakdown • Surge voltage – The maximum dc voltage that can be applied for a short period of time • Leakage current – The current that results in the total discharge of a capacitor as the capacitor is disconnected from the charging network for a sufficient length of time.

  16. Voltage Rating of Capacitors • If the voltage applied across the capacitor is too great, the dielectric will break down and arcing will occur between the capacitor plates. • The voltage rating of the capacitor is the maximum voltage that can be steadily applied without danger of breaking down the dielectric.

  17. Energy Stored by a Capacitor • The ideal capacitor does not dissipate any energy supplied to it. It stores the energy in the form of an electric field between the conducting surfaces. • Charging of a capacitor always involves some expenditure of energy by the charging agency. • This energy is stored up in the electrostatic field set up in the dielectric medium. • On discharging the capacitor, the field collapses and the stored energy is released.

  18. when the capacitor is uncharged, • little work is done in transferring charge from one plate to another. • Let us find the energy spent in charging a capacitor of capacitance C to a voltage V.

  19. Schematic of simple circuit with capacitor

  20. Capacitor Charging

  21. Capacitor Charging Current stops when capacitor is fully charged

  22. Capacitor Charging Capacitor remains charged when power source is removed

  23. R R Charging of Capacitors • As a capacitor becomes charged, the current flow decreases because the voltage developed by the capacitor increases over time and opposes the source voltage.

  24. Transients in Capacitive Networks: Charging Phase • The placement of charge on the plates of a capacitor does not occur instantaneously. • Transient Period – A period of time where the voltage or current changes from one steady-state level to another. • The current ( ic ) through a capacitive network is essentially zero after five time constants of the capacitor charging phase.

  25. Initial Conditions • The voltage across a capacitor at the instant of the start of the charging phase is called the initial value. Once the voltage is applied the transient phase will commence until a leveling off occurs after five time constants called steady-state as shown in the figure.

  26. I Vc or Q t t Charging a Capacitor • Voltage-charge characteristics • Current flow

  27. Capacitor Discharging Capacitor discharges when a current path is applied

  28. Capacitor Discharging Capacitor discharges when a current path is applied

  29. Capacitor Discharging Capacitor discharges when a current path is applied

  30. Capacitor Discharging Capacitor discharges when a current path is applied

  31. Capacitor Discharging Capacitor discharges when a current path is applied

  32. Capacitor Discharging Capacitor discharges when a current path is applied

  33. Capacitor Discharging Capacitor is fully discharged when plates are neutral

  34. R R Discharging of Capacitors • The charged capacitor is the source of voltage for the current flow. The current will cease flowing when the charges of the two plates are again equal, meaning that the capacitor is completely discharged.

  35. t VC or Q I t Discharging a Capacitor • Voltage-charge characteristics • Current flow

  36. Time Constant • Resistance is unavoidable in circuits, through the wire itself or through components such as resistors. • Resistance introduces the element of time into charging and discharging a capacitor • The voltage across a capacitor cannot change instantaneously because it takes finite time to move charge from one point to another. • The rate at which a capacitor charges or discharges is determined by the time constant t = RC (seconds) • During one time constant interval, the charge on a capacitor changes approx. 63% • Five time constant intervals is accepted as the time to fully charge or discharge a capacitor and is called the transient time.

  37. Charging Capacitor Voltage appliedvoltage chargevoltage Time

  38. Charging Capacitor Voltage appliedvoltage resistance added chargevoltage Time

  39. Discharging Capacitor Voltage appliedvoltage chargevoltage Time

  40. Discharging Capacitor Voltage appliedvoltage resistance added chargevoltage Time

  41. Applications • Capacitors find applications in: • Electronic flash lamps for cameras • Line conditioners • Timing circuits • Electronic power supplies

  42. Applications of Capacitors • The capacitance is varied by • altering the overlap between • a fixed set of metal plates • and a moving set. These are • used to tune radio receiver. • Press the key on a computer keyboard reduce the capacitor spacing thus increasing the capacitance which can be detected electronically.

  43. Applications of Capacitors • Capacitivetouch-screens use a layer of capacitive material to hold an electrical charge; touching the screen changes the amount of charge at a specific point of contact.

  44. THE END

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