Deriving a Limit from a Differential Equation: Is It Valid?

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The discussion revolves around the validity of deriving the limit lim k->0 (e^kt-a)/k = at from a differential equation. Initial attempts at the derivation faced confusion over the treatment of constants and the application of L'Hôpital's Rule. It was clarified that the limit does not hold unless specific conditions are met, particularly when a=1. The importance of correctly handling integration constants was emphasized, as they depend on initial conditions and cannot be treated as arbitrary. Ultimately, the conclusion is that the original limit is not valid without further constraints.
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Sorry, I don't know how to write this besides just plain text, but it shouldn't be too hard to read:

lim k->0 (e^kt-a)/k = at

It seems strange to me, and I have no idea how to derive it. Here's how I got it. Starting with:

dv/dt = a+kv

Seperate variables and integrate to get:

dv/(a+kv) = dt

(1/k)*ln(a+kv) = t+c (I'll set c=0 from here on)

a+kv = e^(kt)

v = (e^kt-a)/k

which is the left side of the limit. But as k goes to 0 in the original equation:

dv/dt = a

v = at

Is this right? If so, is there a better way to derive it? If not, where did I go wrong? (I know there are multiple divide by zeros, but I don't think that's the problem because k varies continuously, and the original curve could get closer and closer to a straight line as k is smaller and smaller but still greater than 0.)
 
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I think you mistyped your original equation but I think you're looking for l'Hopital's Rule, i.e. the limit of the ratio is the same as the limit of the ratio of the derivatives when both numerator and denominator of the original ratio tend to zero (simplified version!)
 
I don't think I mistyped. I derive it below, is there a mistake there?
 
I'm having trouble understanding your very first equation and wonder what v is.
 
Do you mean e^(kt-a)/k or (e^(kt)- a)/k??

In any case, I don't see that this has a limit. In the first case, the numerator approaches e^(-a) while the denominator goes to 0. In the second case, the numerator goes to 1-a while the denominator goes to 0.

Whatever the problem is, whether you are trying L'Hopital's rule or not, there is no point in differentiating with respect to t. The only parameter being varied is k.

You CAN show that lim(k->0)(e^(kt)- 1)/k= t by using L'Hopital's rule (differentiating with respect to k) and so you might intend showing that
lim(k->0)(e^(kat)-1)/k= at.
 
so you might intend showing that
lim(k->0)(e^(kat)-1)/k= at

Either that or
lim k->0 (ae^kt-a)/k = at,
but certainly the limit as originally posted is not valid.
 
You're right, there should be an a in front of e^kt. I set c=0 thinking it wouldn't matter, but that's the difference. Now it works with l'hopitals rule. Still, if you go through my derivation, it seems like the limit should still equal at+c for some c. Is that true?

By the way, I'm sorry if this was confusing. a and t are just parameters, and v is only used in the derivation. I adapted this from a physics problem (a was acceleration(gravity), k was the drag coefficient, etc.) where I was looking at how ideal motion is acheived as k->0. Maybe in that context it makes more sense, but I did change a few things so don't thake that too seriously.
 
Erm, well, if the limit exists, then yes, trivially there is some c such that the limit l, equals at+c, c=l-at for instance.
 
Here's what I was trying to say. I learned a little tex code to make it easier to read. This was the original limit:

\lim_{k \rightarrow 0} \\ \frac{e^{kt}-a}{k} = at

However, I made a mistake in the derivation, not treating the constant of integration correctly, and thought it should be modified to this:

\lim_{k \rightarrow 0} \\ \frac{C_{1}e^{kt}-a}{k} = at+C_{2}

But I didn't really think this through either, assuming the constants were completely arbitrary and that whatever I pick for C_{1} (eg., 1, to get back my original limit), I could find another number for C_{2} that would make the limit valid. Now I realize what the problem is. Here is my work:

\frac{dv}{dt} = k v+a

\frac{dv}{k v+a} = dt

Last time, I did two indefinite integrals with a constant, but since that didn't seem to work right, I tried it like this:

\int_{v_{0}}^{v} \frac{dv'}{k v'+a} = \int_{0}^{t} dt'

where v=v(t) and v_{0}=v(0)

\frac{1}{k} (\ln(k v'+a)\mid_{v_{0}}^{v})= t

\ln(k v+a)-\ln(k v_{0}+a)= k t

\ln(\frac{k v+a}{k v_{0}+a})= k t

\frac{k v+a}{k v_{0}+a}= e^{k t}

k v+a=(k v_{0}+a) e^{k t}

v(t)=\frac{(k v_{0}+a) e^{k t}-a}{k}

Now you can see why the constant is not completely arbitrary. It depends not only on the initial conditions, but also on k, so it cannot be treated as an independent parameter in the limit.

\lim_{k \rightarrow 0} \ \frac{(k v_{0}+a) e^{k t}-a}{k}

= \lim_{k \rightarrow 0} \ \frac{v_{0} (k e^{k t})+a (e^{k t}-1)}{k}

This is 0/0, so by l'hopitals rule, you can differentiate the top and bottom to get:

=\lim_{k \rightarrow 0} \ \frac{v_{0} (k t e^{k t}+e^{k t})+a(t e^{k t})}{1}

= v_{0} (0+1)+a(t (1))

= at+v_{0}


So replacing v_{0} with C, the limit I was looking for is:

\lim_{k \rightarrow 0} \ \frac{(k C + a) e^{k t}-a}{k} = at+C

This is valid, right? Thanks for the help everyone.
 
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  • #10
The whole premise is wrong. Asking what the orginal limit is is meaningless unless a=1, obviously the limit doesn't exist unless a=1. Forget about finding these constants which is dubious at best.
 
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