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SMU PHYS 1304 - Force

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Slide 1Chapter 26Capacitors = that which have capacitance to hold = containersCapacitanceMore About CapacitanceCapacitance of a one conductor system is small: for example, Isolated SphereHow to Make a Capacitor?A Real Parallel Plate Capacitor charged up with a battaryOther type of capacitors a Cylindrical CapacitorEnergy stored in a charged capacitorHow Much Energy Stored in a CapacitorEnergy in a Capacitor, the formulaEnergy in a Capacitor, final discussionCapacitors with DielectricsDielectrics, contDielectrics, finalSlide 17Types of Capacitors – TubularTypes of Capacitors – Oil FilledTypes of Capacitors – ElectrolyticTypes of Capacitors – VariableDielectrics – An Atomic ViewDielectrics – An Atomic View, 2Dielectrics – An Atomic View, 3Dielectrics – An Atomic View, 4Dielectrics – An Atomic View, finalInduced Charge and FieldChargespositive (+) negative (-)conservationForce (field)Potential (energy)121212rrF221022141rqqrqqkeForce between point chargeseq=F Er rForce on charge in the field0AEqdEConnect field with its source: chargeBAdV sEqVU Connect field with energyWhat for?To understand the worldOr to move on to capacitor, one of the three passive components in circuitsChapter 26Capacitance andDielectricsCapacitors = that which have capacitance to hold = containersCapacitors are devices that store electric chargeAny conductors can store electric charge, butCapacitors that specially designed devices to story a lot of chargesExamples of where capacitors are used include:radio receiversfilters in power suppliesto eliminate sparking in automobile ignition systemsenergy-storing devices in electronic flashesHow is my English?CapacitanceThe capacitance, C, is defined as the ratio of the amount of the charge Q on the conductor to the potential increase ΔV of the conductor because of the charge:This ratio is an indicator of the capability that the object can hold charges. It is a constant once the object is given, regardless there is charge on the object or not. This is like the capacitance of a mug which does not depend on there is water in it or not. The SI unit of capacitance is the farad (F)VQCQVC=1V1C F1 More About CapacitanceCapacitance will always be a positive quantityThe capacitance of a given capacitor is constantThe capacitance is a measure of the capacitor’s ability to store chargeThe farad is an extremely large unit, typically you will see microfarads (F=10-6F), nanofarads (nF=10-19F), and picofarads (pF=10-12F)Capacitance of a one conductor system is small: for example, Isolated SphereAssume a spherical charged conductor with radius RThe sphere will have the same capacitance as it would if there were a conducting sphere of infinite radius, concentric with the original sphereAssume V = 0 for the infinitely large shellEven for R=1m, C = 0.1 nFNote, this is independent of the charge and the potential differenceeekRRQkQVQC How to Make a Capacitor?Requirements:Hold chargesThe potential increase does not appear outside of the device, hence no influence to other devices.Is there such a good thing?For this parallel plate capacitor, the capacitance isarea surface theis ,00AdAdAEdAVQC02 E0022 E0E0E0EdEdV Quiz x: Isn’t Physics easy once you really understand it?A Real Parallel Plate Capacitor charged up with a battaryEach plate is connected to a terminal of the batteryThe battery is a source of potential differenceIf the capacitor is initially uncharged, the battery establishes an electric field in the connecting wiresThis field applies a force on electrons in the wire just outside of the platesThe force causes the electrons to move onto the negative plateThis continues until equilibrium is achievedThe plate, the wire and the terminal are all at the same potentialAt this point, there is no field present in the wire and the movement of the electrons ceasesThe plate is now negatively chargedA similar process occurs at the other plate, electrons moving away from the plate and leaving it positively chargedIn its final configuration, the potential difference across the capacitor plates is the same as that between the terminals of the batteryVOther type of capacitorsa Cylindrical CapacitorV = -2ke  ln (b/a) = Q/lThe capacitance is( )2 ln /eQCV k b a= =DlEnergy stored in a charged capacitor Consider the circuit to be a systemBefore the switch is closed, the energy is stored as chemical energy in the batteryWhen the switch is closed, the energy is transformed from chemical to electric potential energyThe electric potential energy is related to the separation of the positive and negative charges on the platesA capacitor can be described as a device that stores energy as well as chargeHow Much Energy Stored in a Capacitorq -qdqTo study this problem, recall that the work the field force does equals to the electric potential energy loss:VQUWEEVdqCqVdqdWBWhen the charge buildup is q, move a dq, the work isThis also means that when the battery moves a charge dq to charge the capacitor, the work the battery does equals to the buildup of the electric potential energy:UWBWe now have the answer to the final charge Q: UCQdqCqdWWQQBB2200Energy in a Capacitor, the formulaWhen a capacitor has charge stored in it, it also stores electric potential energy that isThis applies to a capacitor of any geometryThe energy stored increases as the charge increases and as the potential difference increasesIn practice, there is a maximum voltage before discharge occurs between the plates22)(212VCCQUEEnergy in a Capacitor, final discussionThe energy can be considered to be stored in the electric field For a parallel-plate capacitor, the energy can be expressed in terms of the field as U = ½ (εoAd)E2It can also be expressed in terms of the energy density (energy per unit volume)uE = ½ E2Capacitors with DielectricsA dielectric is a nonconducting material that, when placed between the plates of a capacitor, increases the capacitanceDielectrics include rubber, glass, and waxed paperWith a dielectric, the capacitance becomes C = κCo The capacitance increases


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SMU PHYS 1304 - Force

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