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Capacitors Part I

Capacitors Part I. Capacitor. Composed of two metal plates. Each plate is charged one positive one negative Stores Charge. SYMBOL. A simple Capacitor. TWO PLATES. WIRES. Battery. INSIDE THE DEVICE. d. Air or Vacuum. E. - Q +Q. Symbol. Area A.

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Capacitors Part I

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  1. Capacitors Part I

  2. Capacitor • Composed of two metal plates. • Each plate is charged • one positive • one negative • Stores Charge SYMBOL

  3. A simple Capacitor TWO PLATES WIRES Battery

  4. INSIDE THE DEVICE

  5. d Air or Vacuum E - Q +Q Symbol Area A V=Potential Difference Two Charged Plates(Neglect Fringing Fields) ADDED CHARGE

  6. Where is the charge? +++++ + - - - - - - d AREA=A s=Q/A Air or Vacuum E - Q +Q Area A V=Potential Difference

  7. One Way to Charge: • Start with two isolated uncharged plates. • Take electrons and move them from the + to the – plate through the region between. • As the charge builds up, an electric field forms between the plates. • You therefore have to do work against the field as you continue to move charge from one plate to another. The capacitor therefore stores energy!

  8. Capacitor Demo

  9. d Air or Vacuum E - Q +Q Gaussian Surface Area A V=Potential Difference More on Capacitors Same result from other plate!

  10. DEFINITION • The Potential Difference is APPLIED by a battery or a circuit. • The charge q on the capacitor is found to be proportional to the applied voltage. • The proportionality constant is C and is referred to as the CAPACITANCE of the device.

  11. NOTE • Work to move a charge from one side of a capacitor to the other is qEd. • Work to move a charge from one side of a capacitor to the other is qV • Thus qV=qEd • E=V/d (Hold this thought.)

  12. UNITS • A capacitor which acquires a charge of 1 coulomb on each plate with the application of one volt is defined to have a capacitance of 1 FARAD • One Farad is one Coulomb/Volt

  13. Continuing… • The capacitance of a parallel plate capacitor depends only on the Area and separation between the plates. • C is dependent only on the geometry of the device!

  14. Units of e0 pico

  15. Simple Capacitor Circuits • Batteries • Apply potential differences • Capacitors • Wires • Wires are METALS. • Continuous strands of wire are all at the same potential. • Separate strands of wire connected to circuit elements may be at DIFFERENT potentials.

  16. Size Matters! • A Random Access Memory stores information on small capacitors which are either charged (bit=1) or uncharged (bit=0). • Voltage across one of these capacitors ie either zero or the power source voltage (5.3 volts in this example). • Typical capacitance is 55 fF (femto=10-15) • Question: How many electrons are stored on one of these capacitors in the +1 state?

  17. Small is better in the IC world!

  18. TWO Types of Connections SERIES PARALLEL

  19. V CEquivalent=CE Parallel Connection

  20. q -q q -q V C1 C2 Series Connection The charge on each capacitor is the same !

  21. q -q q -q V C1 C2 Series Connection Continued

  22. More General

  23. Example C1=12.0 uf C2= 5.3 uf C3= 4.5 ud C1 C2 series (12+5.3)pf (12+5.3)pf V C3

  24. E=e0A/d +dq +q -q More on the Big C • We move a charge dq from the (-) plate to the (+) one. • The (-) plate becomes more (-) • The (+) plate becomes more (+). • dW=Fd=dq x E x d

  25. So….

  26. Parallel Plate Cylindrical Spherical Not All Capacitors are Created Equal

  27. Spherical Capacitor

  28. Calculate Potential Difference V (-) sign because E and ds are in OPPOSITE directions.

  29. Continuing… Lost (-) sign due to switch of limits.

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