nelsyeung
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I've started an experiment lately with charging a capacitor through a resistor, I wanted to prove that the equation of charging capacitor by using linear law, but it didn't quite work and needed help.
This is what I've done:
Equation of charging a capacitor:
V = V_{max}(1-e^{\frac{-t}{RC}})
Multiply out of bracket:
V = V_{max} - V_{max} e^{\frac{-t}{RC}}
Apply natural log to remove the e:
ln(V) = ln(V_{max}) - ln(V_{max} e^{\frac{-t}{RC}})
Use laws of logs and ln(e) will cancels out:
ln(V) = ln(V_{max}) - ln(V_{max}) + \frac{-t}{RC}
ln(V_{max}) - ln(V_{max}) = 0, therefore:
ln(V) = \frac{-t}{rc}
So this tells me if I plot a graph with ln(V) against t, I should get a straight line, but it doesn't, the new graph looks identical to the first graph I drew only with different values, and also I found out that using that formula created by linear law, I can seem to get it back to the original equation.. :( Please help.
Thanks, Nels
This is what I've done:
Equation of charging a capacitor:
V = V_{max}(1-e^{\frac{-t}{RC}})
Multiply out of bracket:
V = V_{max} - V_{max} e^{\frac{-t}{RC}}
Apply natural log to remove the e:
ln(V) = ln(V_{max}) - ln(V_{max} e^{\frac{-t}{RC}})
Use laws of logs and ln(e) will cancels out:
ln(V) = ln(V_{max}) - ln(V_{max}) + \frac{-t}{RC}
ln(V_{max}) - ln(V_{max}) = 0, therefore:
ln(V) = \frac{-t}{rc}
So this tells me if I plot a graph with ln(V) against t, I should get a straight line, but it doesn't, the new graph looks identical to the first graph I drew only with different values, and also I found out that using that formula created by linear law, I can seem to get it back to the original equation.. :( Please help.
Thanks, Nels