Motion along a stretching band

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SUMMARY

The problem involves an ant crawling at 1 foot/second on a rubber band that stretches at 1 foot/second, starting from an original length of 2 feet. The length of the band at time t is expressed as t + 2. The ant's progress is modeled by the fraction y(t), leading to the equation y' = 1/(t + 2) and the solution y = ln(t + 2) - ln(2). Ultimately, the time T when the ant reaches the end of the band is calculated as T = 2e - 2.

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This was given as a problem in a calculus textbook I'm working through (apologies if this should have gone in the physics forum)

1. Homework Statement

An ant crawls at 1foot/second along a rubber band whose
original length is 2 feet. The band is being stretched at 1
foot/second by pulling the other end. At what time T, if ever,
does the ant reach the other end?
One approach: The band's length at time t is t + 2. Let y(t)
be the fraction of that length which the ant has covered, and
explain
(a) y' = 1/(t + 2) (b)y =ln(t + 2) -ln 2 (c) T = 2e -2.

Homework Equations


∫1/x dx = ln(x)

The Attempt at a Solution


Given a, I can get to b by integrating and finding the constant, and then to c by solving for y=1, but I'm stumped on how to get to explain a. y' seems to be the ant's speed over the length of the band, by I don't understand why that is so.
 
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Calculus by Gilbert Strang? :woot: I read that one too.

y' is the rate of change of the fraction which has been traversed. Suppose the ant was not crawling: when the rubber band is being stretched, the fraction of the rubber band behind the ant would not change (because it also stretches).
 
Yup.

I see that y' is the rate of change of the fraction, but I'm still not sure why why it equals what it does.
 
Consider two special cases to try to get an intuition:

The case where the ant is not crawling (but starts out at some initial fraction y0).
The case where the rubber band is a fixed length.

What would the equation for y' be in each of these (separate) cases?
 
Got it, Thanks.
 

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