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Energy Stored in a Charged Capacitor

发布时间:2026-08-22 | 浏览:1
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Classification of Magnetic Materials Hysteresis: Retentivity and Coercivity Permanent Magnet Magnetic Shielding Overview: Magnetic Materials Electromagnetic Induction Introduction to Electromagnetic Induction Faraday's Laws of Electromagnetic Induction Lenz's Law Flux of a Vector Field Motional Electromotive Force (e.m.f.) Induced Emf in a Stationary Coil in a Changing Magnetic Field Generators Back Emf and Back Torque Induction and Energy Transfer Eddy Currents or Foucault Currents Self Inductance Energy Stored in a Magnetic Field Energy Density of a Magnetic Field Mutual Inductance Transformers Overview of Electromagnetic Induction Introduction to Electromagnetic Induction Faraday's Laws of Electromagnetic Induction Flux of a Vector Field Motional Electromotive Force (e.m.f.) Induced Emf in a Stationary Coil in a Changing Magnetic Field Back Emf and Back Torque Induction and Energy Transfer Eddy Currents or Foucault Currents Self Inductance Energy Stored in a Magnetic Field Energy Density of a Magnetic Field Mutual Inductance Overview of Electromagnetic Induction Electrostatics Mechanical Force on Unit Area of a Charged Conductor Energy Density of a Medium Concept of Condenser The Parallel Plate Capacitor Capacity of Parallel Plate Condenser Effect of Dielectric on Capacitance Energy of Charged Condenser Condensers in Series and Parallel, Van-deGraaff Generator Mechanical Force on Unit Area of a Charged Conductor Energy Density of a Medium Concept of Condenser The Parallel Plate Capacitor Capacity of Parallel Plate Condenser Effect of Dielectric on Capacitance Energy of Charged Condenser Condensers in Series and Parallel, Van-deGraaff Generator AC Circuits Introduction to Ac and Aс Circuits Values of Alternating Current Phasors AC Voltage Applied to a Resistor AC Voltage Applied to an Inductor AC Voltage Applied to a Capacitor AC Voltage Applied to a Series LCR Circuit Power in AC Circuit LC Oscillations Electric Resonance Sharpness of Resonance: Q Factor Choke Coil Overview: AC Circuits Introduction to Ac and Aс Circuits Values of Alternating Current AC Voltage Applied to a Resistor AC Voltage Applied to an Inductor AC Voltage Applied to a Capacitor AC Voltage Applied to a Series LCR Circuit Power in AC Circuit LC Oscillations Electric Resonance Sharpness of Resonance: Q Factor Overview: AC Circuits Current Electricity Meter Bridge Dual Nature of Radiation and Matter Understanding Dual Nature of Radiation and Matter The Photoelectric Effect Wave-particle Duality of Electromagnetic Radiation Photo Cell De Broglie Hypothesis Davisson and Germer Experiment Wave-particle Duality of Matter Overview: Dual Nature of Radiation and Matter Understanding Dual Nature of Radiation and Matter The Photoelectric Effect Wave-particle Duality of Electromagnetic Radiation De Broglie Hypothesis Davisson and Germer Experiment Wave-particle Duality of Matter Overview: Dual Nature of Radiation and Matter Magnetic Effects of Electric Current Ampere’s Circuital Law Moving Coil Galvanometer Cyclotron Ampere’s Circuital Law Moving Coil Galvanometer Magnetism Current Loop as a Magnetic Dipole : Magnetic Dipole Moment of Current Loop Magnetic Dipole Moment of a Revolving Electron Magnetisation and Magnetic Intensity Magnetic Properties of Materials Curie Temperature Current Loop as a Magnetic Dipole : Magnetic Dipole Moment of Current Loop Magnetic Dipole Moment of a Revolving Electron Magnetisation and Magnetic Intensity Magnetic Properties of Materials Curie Temperature Structure of Atoms and Nuclei Structure of the Atom and Nucleus Thomson’s Atomic Model Geiger-marsden Experiment Rutherford’s Atomic Model Atomic Spectra Neils Bohr’s Model of an Atom Atomic Nucleus Constituents of a Nucleus Isotopes Atomic and Nuclear Masses Size of the Nucleus Mass Defect and Binding Energy Binding Energy Curve Forms of Energy > Nuclear Energy Nuclear Binding Energy Radioactive Decays Law of Radioactive Decay Overview: Structure of Atoms and Nuclei Structure of the Atom and Nucleus Thomson’s Atomic Model Geiger-marsden Experiment Rutherford’s Atomic Model Neils Bohr’s Model of an Atom Constituents of a Nucleus Atomic and Nuclear Masses Size of the Nucleus Mass Defect and Binding Energy Binding Energy Curve Forms of Energy > Nuclear Energy Nuclear Binding Energy Radioactive Decays Law of Radioactive Decay Overview: Structure of Atoms and Nuclei Semiconductor Devices Basics of Semiconductor Devices p-n Junction Diode as a Rectifier Special Purpose P-n Junction Diodes Bipolar Junction Transistor (BJT) Logic Gates Overview: Semiconductor Devices Basics of Semiconductor Devices p-n Junction Diode as a Rectifier Special Purpose P-n Junction Diodes Bipolar Junction Transistor (BJT) Overview: Semiconductor Devices Electromagnetic Inductions Introduction to Electromagnetic Induction Self Inductance Mutual Inductance Transformers Need for Displacement Current Coil Rotating in Uniform Magnetic Induction Alternating-Current Generator Reactance and Impedance LC Oscillations Inductance and Capacitance Resonant Circuits Power in AC Circuit Lenz’s Law and Conservation of Energy Introduction to Electromagnetic Induction Self Inductance Mutual Inductance Need for Displacement Current Coil Rotating in Uniform Magnetic Induction Alternating-Current Generator Reactance and Impedance LC Oscillations Inductance and Capacitance Resonant Circuits Power in AC Circuit Lenz’s Law and Conservation of Energy Electrons and Photons Photoelectric Effect - Hertz’s Observations Photoelectric Effect - Hallwachs’ and Lenard’s Observations Einstein’s Equation - Particle Nature of Light Particle Nature of Light Photoelectric Effect - Hertz’s Observations Photoelectric Effect - Hallwachs’ and Lenard’s Observations Einstein’s Equation - Particle Nature of Light Particle Nature of Light Atoms, Molecules and Nuclei Alpha-particle Scattering and Rutherford’s Nuclear Model of Atom Bohr’s Model for Hydrogen Atom Hydrogen Spectrum Atomic Masses and Composition of Nucleus Radioactivity Law of Radioactive Decay Atomic Mass, Mass - Energy Relation and Mass Defect Nuclear Binding Energy Nuclear Fusion de-Broglie Relation Wave Nature of Matter Wavelength of an Electron Davisson and Germer Experiment Continuous and Characteristics X-rays Mass Defect and Binding Energy Alpha-particle Scattering and Rutherford’s Nuclear Model of Atom Bohr’s Model for Hydrogen Atom Hydrogen Spectrum Atomic Masses and Composition of Nucleus Law of Radioactive Decay Atomic Mass, Mass - Energy Relation and Mass Defect Nuclear Binding Energy de-Broglie Relation Wave Nature of Matter Wavelength of an Electron Davisson and Germer Experiment Continuous and Characteristics X-rays Mass Defect and Binding Energy Semiconductors Energy Bands in Materials Extrinsic Semiconductor Applications of n-type and p-type Semiconductors Special Purpose P-n Junction Diodes Semiconductor Diode Voltage Regulator I-V Characteristics of Led Transistor and Characteristics of a Transistor Transistor as an Amplifier (Ce-configuration) Transistor as a Switch Oscillators Digital Electronics and Logic Gates Energy Bands in Materials Extrinsic Semiconductor Applications of n-type and p-type Semiconductors Special Purpose P-n Junction Diodes Semiconductor Diode Voltage Regulator I-V Characteristics of Led Transistor and Characteristics of a Transistor Transistor as an Amplifier (Ce-configuration) Transistor as a Switch Digital Electronics and Logic Gates Communication Systems Basic Terminology Used in Electronic Communication Systems Bandwidth of Signals Bandwidth of Transmission Medium Need for Modulation and Demodulation Production and Detection of an Amplitude Modulated Wave Space Communication Propagation of EM Waves Modulation and Its Necessity Basic Terminology Used in Electronic Communication Systems Bandwidth of Signals Bandwidth of Transmission Medium Need for Modulation and Demodulation Production and Detection of an Amplitude Modulated Wave Space Communication Propagation of EM Waves Modulation and Its Necessity A capacitor stores electrical potential energy when it is charged. This energy is associated with the electric field set up between its plates, not merely with charge “sitting” on the plates. A useful analogy is a water tank being filled against gravity: as the water level rises, further filling requires more work. In the same way, as a capacitor charges, the potential difference rises, so adding more charge requires increasing work. Definition: Energy Stored in a Capacitor The work done in the transfer of charge q between the two plates of a capacitor, which gets stored in the form of potential energy of the system, is called the energy stored in a capacitor. Formula: Energy Stored / Work Done in a Capacitor W = \[\frac {1}{2}\]qV U = \[\frac {Q^2}{2C}\] ​= \[\frac {1​}{2}\]QV = \[\frac {1}{2}\]​CV 2 SI unit: Joule (J) Stepwise Derivation Consider a capacitor of capacitance C. At some intermediate stage of charging, let the charge on it be q. Then the potential difference across it is: V = \[\frac {q}{C}\] If an additional small charge dq is supplied, the small work done is: dW = V dq = \[\frac {q}{C}\]dq Total work done in charging the capacitor from 0 to the final charge Q is: W = \[\int_0^Q\frac{q}{C}dq\] W = \[\frac{1}{C}\int_0^Qqdq=\frac{1}{C}\left[\frac{q^2}{2}\right]_0^Q\] W = \[\frac{Q^2}{2C}\] Since this work is stored as energy: U = \[\frac{Q^2}{2C}\]​ Using Q = CV, the equivalent forms become: U = \[\frac{Q^2}{2C}=\frac{1}{2}QV=\frac{1}{2}CV^2\] The energy stored in a charged capacitor is actually stored in the electric field between its plates. For a parallel-plate capacitor, the energy density of the electric field is: where u is energy per unit volume, and E is electric field intensity. Energy density indicates how much electrical energy is stored per unit volume of the field. This is an important bridge between electrostatics and field-based physics. A parallel-plate capacitor (3 × 10⁻⁹ F) is connected to 400 V. A dielectric slab (K = 3, thickness 3 cm) completely fills the space. The voltage is kept constant. What is the change in energy when the slab is removed? At constant voltage, energy U = \[\frac {1}{2}\]CV 2 , so energy ∝ capacitance. Steps in simple words With air: use given C = 3 × 10⁻⁹ F and V = 400 V. U air = \[\frac {1}{2}\]CV 2 = 24 × 10 −5 J. With dielectric: new capacitance C′ = kC = 3 × 3 × 10 −9 = 9 × 10 −9 F. U dielectric = \[\frac {1}{2}\]C′V 2 = 72 × 10 −5 J. Change in energy = U dielectric − U air = (72 − 24) × 10 −5 = 48 × 10 −5 J. Conclusion in one line: When the dielectric is present, energy is higher by 48 × 10 −5 J at constant voltage. (a) A 900 pF capacitor is charged by 100 V. Find the stored energy. (b) Then it is disconnected and connected to another 900 pF capacitor (uncharged). Find a new total energy. Capacitance C = 900 pF = 900 × 10 −12 F, voltage V = 100 V. Charge: Q = CV = 900 × 10 −12 × 100 = 9 × 10 −8 C. Energy: U = \[\frac {1}{2}\]CV 2 = \[\frac {1}{2}\]QV. U = \[\frac {1}{2}\] × 9 × 10 −8 × 100 = 4.5 × 10 −6 J. Simple meaning: This is how much energy the single capacitor stores when charged to 100 V. Now two equal capacitors (both 900 pF) are connected, so the final charges are shared equally. Let the final potential be V′. Then each capacitor has Q′ = CV′. Total charge is conserved: Q total = Q. So each gets Q′ = Q/2. Therefore V′ = Q′/C = (Q/2)/C = V/2. Energy in each capacitor: \[\frac {1}{2}\]Q′V′. Total energy = 2 × \[\frac {1}{2}\]Q′V′ = Q′V′ = \[\frac {1}{4}\]QV. Numerically: U final = 2.25 × 10 −6 J. Final energy is half of the initial: 4.5 × 10 −6 → 2.25 × 10 −6 J. The “missing” energy is lost as heat and electromagnetic radiation when charge flows during connection. Shaalaa.com | Capacitor and Capacitance part 19 (Energy Stored in Capacitors, Energy density) Related Questions VIEW ALL [45] Two capacitors of capacitances 4⋅0 µF and 6⋅0 µF are connected in series with a battery of 20 V. Find the energy supplied by the battery. A 12 pF capacitor is connected to a 50 V battery. How much electrostatic energy is stored in the capacitor? Consider the situation shown in figure. The switch is closed at t = 0 when the capacitors are uncharged. Find the charge on the capacitor C 1 as a function of time t. A capacitor of capacitance 12.0 μF is connected to a battery of emf 6.00 V and internal resistance 1.00 Ω through resistanceless leads. 12.0 μs after the connections are made, what will be (a) the current in the circuit (b) the power delivered by the battery (c) the power dissipated in heat and (d) the rate at which the energy stored in the capacitor is increasing? Prove that, if an insulated, uncharged conductor is placed near a charged conductor and no other conductors are present, the uncharged body must be intermediate in potential between that of the charged body and that of infinity. An air-filled parallel plate capacitor has a uniform electric field `overset(->)("E")` in the space between the plates. If the distance between the plates is 'd' and the area of each plate is 'A', the energy stored in the capacitor is ______ (∈ 0 = permittivity of free space) Obtain the expression for the energy stored per unit volume in a charged parallel plate capacitor. A 20 μF capacitor is joined to a battery of emf 6.0 V through a resistance of 100 Ω. Find the charge on the capacitor 2.0 ms after the connections are made. 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