the charge on a capacitor in a circuit containing C,a resistance R,and a source of voltage E is given by q=CE(1-e^(-t/RC)).show that this satisfies the equation Rdq/dt+q/C=E
Hint: If I compute the first derivative of the function \(\Large q(t)\), then I get: \[\Large \frac{{dq}}{{dt}} = EC \cdot \frac{1}{{RC}}\exp \left( { - \frac{t}{{RC}}} \right)\] please substitute that first derivative, together the same function \(\Large q(t)\) into your differential equation, you should get an identity
Is that exp the same as e?
e as in the opposite of a natural log?
yes
Thank you :)
no, thank "the maestro"
Thank both of you lol. You helped too :) I had no idea what exp meant. Shows how much I know about claculus :/
To find that derivative, did you first distribute the CE and then use d/dx e^x=e^x * x^i?
@IrishBoy123 @Michele_Laino
hey ruby, i think we started with: \[\Large q(t)=CE(1-e^{\frac{-t}{RC}})\] and we have to show that \(\Large R\dot q+\dfrac{q}{C}=E\) is true |dw:1448836931798:dw|
Yes I'm just not sure how we got to|dw:1448836976942:dw|
I'm sorry if I seem incompetent lol.
ruby, are you online now???
Yes
cool did we get the first bit right: \(\large q(t)=CE(1-e^{\frac{-t}{RC}})\) ??
Yes, and you're correct in stating that we need to prove that \[q=CE(1-e ^{-t/RC}) \] satisfies the second equation
so we need : \(\large \dot q(t)=CE \dfrac{d}{dt}\left\{(1-e^{\frac{-t}{RC}})\right\}\)
Would you distribute the CE and then use the chain rule theorem?
the CE is a constant. keep it outside.
Alright, so just use chain rule on e^-t/RC?
\(\large \dfrac{d}{dt}(1-e^{\frac{-t}{RC}}) = \dfrac{d}{dt}(1)-\dfrac{d}{dt}e^{\frac{-t}{RC}}) \)
\(\large \dfrac{d}{dt}(e^{-\frac{t}{RC}}) = -\frac{1}{RC}~e^{\frac{-t}{RC}}\)
ruby keep asking, if the answers are not helpful. :p
And then I substitute that into the second equation? And try to get E=E?
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