continuity equation and relaxation time

continuity equation and relaxation time

• 1.
  SUB : FIELDTHEORY TOPIC :Continuity Equation and Relaxation Time 1 GROUP NAME : 1.RAVIJEET VASHI (150990109010) 1.RAVIRAJ SOLANKI (150990109011) Guided by : MS. RICHA DUBEY
• 2.
  Continuity Equation According toprinciple of charge conservation, the time rate of decrease of charge within a given volume must be equal to the net outward current flow through the closed surface of the volume. The current Iout coming out of the closed surface where Qin is the total charge enclosed by the closed surface. Using divergence theorem But (i)
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  Equation (i) nowbecomes This is called the continuity of current equation. Effect of introducing charge at some interior point of a conductor/dielectric or (ii)
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  RELAXATION TIME  Accordingto Ohm’s law  According to Gauss’s law
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  Equation (ii) nowbecomes Integrating both sides or This is homogeneous liner ordinary differential equation. By separating variables we get
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  where (iii)
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   Equation (iii)shows that as a result of introducing charge at some interior point of the material there is a decay of the volume charge density ρv.  The time constant Tr is known as the relaxation time or the relaxation time.  Relaxation time is the time in which a charge placed in the interior of a material to drop to e-1 = 36.8 % of its initial value.  For Copper Tr = 1.53 x 10-19 sec (short for good conductors)  For fused Quartz Tr = 51.2 days (large for good dielectrics)