Conversation started Feb 17, 2020 at 10:51.
Feb 17, 2020 10:51
Question: How many time constants will elapse before the power delivered by the battery drops to half of its maximum value in an RC circuit?
What did I do?:
Found an expression for power delivered by the battery as per our previous discussion as - $P=i^2R$.
Substituted the expression for $i$ the current.
@GuruVishnu hi
@JohnRennie Hi sir :-)
But finally I got the answer to be $\ln 2/2$ instead of $\ln 2$; The problem is entirely simple, and my answer varies from the correct one by a factor of $2$.
So, who is incorrect - HC Verma or Guru Vishnu?
Do you want to go through the calculation?
@JohnRennie I think yes. I'm unable to think of other ways to know the correct answer. Is it possible sir?
I just described the method I used, above.
The starting point is to calculate the current as a function of time. Did you do that?
Feb 17, 2020 10:58
Yes sir. $i=Q_0/RC \times (1-e^{-t/RC})$
Where $Q_0$ is the charge the capacitor would carry after some years.
You can simplify this since $V = Q_0/C$ and $I_0 = V/R$, where $I_0$ is the initial current.
So you get $I(t) = I_0 ( 1 - e^{-t/RC} )$
@JohnRennie Ok sir. Understood.
And the power being supplied by the battery is $P = I(t)V$
So the power falls to half the initial value when the current falls to $I_0/2$ i.e. when $1-e^{-t/RC} = 0.5$
Yes sir. And I see you're getting close to the correct book answer.
Yes, you're going to end up with $t = RC\ln2$
Feb 17, 2020 11:03
But what if we use $P=i^2R$ instead of $P=iV$; we must get the same result right? But I tried a lot of times and got $t=\ln 2/2$.
No, that's giving you the power dissipated in the resistor R not the power being supplied by the battery.
You're ignoring the power being converted into the electric field in the capacitor.
@JohnRennie Ok sir. I can see where I went wrong. But could you explain why a simple substitution of $V=iR$ makes the situation different. I'm unable to understand this point.
The substitution only works at time zero.
@JohnRennie Yes sir. Now understood this completely. Thank you sir :-)
At time zero the voltage across the capacitor is zero because no charge has flowed onto it, and that means the whole voltage $V$ is dropped across the resistor. So the current at time zero is $I_0 = V/R$.
@GuruVishnu cool :-)
Feb 17, 2020 11:09
@JohnRennie Yes sir. May I know how were you so careful on the first try itself?
@GuruVishnu I'm not sure what you're asking ...
@JohnRennie How were you so cautious on using $P=iV$ instead of $P=i^2R$ (like me)?
It didn't strike my mind even after a lot of attempts.
I thought of various other scenarios.
The question asks about:
> the power delivered by the battery
Yes sir.
So you need to write down the power delivered by the battery, and this is the battery voltage times the current through the battery. This is true regardless of what the battery is connected to.
Feb 17, 2020 11:13
@JohnRennie Ok sir. Is this true only for ideal batteries or can we extrapolate this to batteries with non-zero internal resistance?
I know the potential must drop with current. But how is this related to power, sir?
It seems, both the $i$ and $V$ terms vary.
If the battery EMF is $E$ then the power produced by the battery is always $P = EI$. But for real batteries some of this power is dissipated in the battery due to the internal resistance $R$.
@JohnRennie Ok sir. I see we can bring the resistor $R$ in the RC circuit into the battery :)
So the power delivered is $P = EI - I^2R$.
@JohnRennie Ok sir. Thank you :-)
 
Conversation ended Feb 17, 2020 at 11:16.