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<strong>www</strong>.<strong>GOALias</strong>.<strong>blogspot</strong>.<strong>com</strong>PhysicsNote that Ad is the volume of the region between the plates (whereelectric field alone exists). If we define energy density as energy storedper unit volume of space, Eq (2.76) shows thatEnergy density of electric field,u =(1/2)ε 0E 2 (2.77)Though we derived Eq. (2.77) for the case of a parallel plate capacitor,the result on energy density of an electric field is, in fact, very general andholds true for electric field due to any configuration of charges.Example 2.10 (a) A 900 pF capacitor is charged by 100 V battery[Fig. 2.31(a)]. How much electrostatic energy is stored by the capacitor?(b) The capacitor is disconnected from the battery and connected toanother 900 pF capacitor [Fig. 2.31(b)]. What is the electrostatic energystored by the system?82EXAMPLE 2.10FIGURE 2.31Solution(a) The charge on the capacitor isQ = CV = 900 × 10 –12 F × 100 V = 9 × 10 –8 CThe energy stored by the capacitor is= (1/2) CV 2 = (1/2) QV= (1/2) × 9 × 10 –8 C × 100 V = 4.5 × 10 –6 J(b) In the steady situation, the two capacitors have their positiveplates at the same potential, and their negative plates at thesame potential. Let the <strong>com</strong>mon potential difference be V′. Thecharge on each capacitor is then Q′ = CV′. By charge conservation,Q′ = Q/2. This implies V′ = V/2. The total energy of the system is1 1−6= 2 × QV ' ' = QV= 2.25×10 J2 4Thus in going from (a) to (b), though no charge is lost; the finalenergy is only half the initial energy. Where has the remainingenergy gone?There is a transient period before the system settles to thesituation (b). During this period, a transient current flows fromthe first capacitor to the second. Energy is lost during this timein the form of heat and electromagnetic radiation.

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