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The theory and steps to calculate the time constant (τ) of an rc circuit using both charging and discharging methods. It includes figures and equations to help understand the concept. The document also suggests completing tables and plotting graphs to determine the value of r1.
Typology: Study notes
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R C
E
S
VR o Vc I
Figure 1:
VR = IR; VC = Q C E − IR −
dQ dt
∫ (^) dQ CE − Q
∫ dt
−ln(CE − Q) = t RC
at t=0 Q = k = −ln(CE)
−ln(CE − Q) =
t RC − ln(CE)
ln(CE − Q) = −
t RC
ln(CE − Q) − ln(CE) = − t RC ln
t RC Q = Qo(1 − e−^ RCt ) CQ = CQo(1 − e−^ RCt ) Vc = Eo(1 − e−^ RCt )
c E (^) o
Eo 2
t 1 t 2 t (time)
τ
τ
τ > τ 2 1
2
1
V
Figure 3:
Vc = Eo(1. 0 − e−^ RCt ) Vc = Eo − Eoe−^ RCt Eo − Vc Eo
= e−^ RCt
ln
o −^ Vc Eo
] = −
t
Complete the following table and plot a graph ln
[ (^) E o−Vc Eo
] vs t. Determine the value for R 1 using this graph and compare your value with previous value for R 1 which was determined in section 2.
Eo(volts) Vc(volts) Eo E−oV c ln
[ (^) E o−Vc Eo
] t(sec)
Vc across the capacitor is shown in figure 4.
c E (^) o
V = E ec (^) o^ −t/RC
t (time)
V
Figure 4:
Vc is given by Vc = Eoe−^ RCt
where Eo is the voltage of the source.
lnVc = −
t + lnEo
Complete the following table and plot a graph lnVc vs t. Determine the value for R 1 using this graph and compare your value with previous value for R 1 which was determined in section 2.
Eo(volts) Vc(volts) ln Vc t(sec)