How can the equation ln(1+d)=d be used to approximate p= Ae^-0.004h/30?

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Discussion Overview

The discussion revolves around the use of the equation ln(1+d) = d to approximate the expression p = Ae^-0.004h/30, particularly in the context of air pressure decay with altitude. Participants explore the mathematical implications of this approximation and its application in modeling air pressure.

Discussion Character

  • Exploratory
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant sketches the curve y = ln x and finds the tangent line at the x-axis, suggesting that for small delta, ln(1+d) is approximately equal to d.
  • Another participant confirms the relationship between the tangent line and the approximation, stating that ln(1 + d) is close to the value on the tangent line when x = 1 + d.
  • A participant questions the meaning of p in the context of the approximation, seeking clarification on the variables involved.
  • Another participant provides a limit definition to demonstrate that ln(1 + d) is approximately equal to d for small d, referencing the concept of derivatives and limits.
  • Several participants reference a previous discussion on the same problem, indicating a shared interest in the tangent line and its implications for the approximation.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the application of the tangent line approximation and the meaning of the variables involved. There is no consensus on how to proceed with the second part of the problem, and multiple viewpoints are presented without resolution.

Contextual Notes

Some participants express confusion about the relationship between the tangent line and the approximation, and there are unresolved questions about the variables and constants in the equation for air pressure.

Bawx
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Hi guys,
I'm having a lot of trouble with this question and any help would be greatly appreciated, thanks!

1. Sketch the curve y = ln x and find the tangent line to this curve at the point where the curve crosses the x-axis. Deduce that, for small delta,

ln(1+d) '=' d

2. Use the approximation from the previous part to deduce that

p = p(h) '=' Ae^-0.004h/30

*the '=' are supposed to be the squiggly approximately signs but I'm not sure how to type those sorry

-I think I've found the equation for the tangent line, as ln(1)=0 and y'=1/x so by using y-y1=m(x-x1) the tangent line is y=x-1 but I'm not sure how this relates to delta at all?

- I'm not really sure how to approach the second part at all

Thanks :)
 
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Bawx said:
Hi guys,
I'm having a lot of trouble with this question and any help would be greatly appreciated, thanks!

1. Sketch the curve y = ln x and find the tangent line to this curve at the point where the curve crosses the x-axis. Deduce that, for small delta,

ln(1+d) '=' d
Good so far. The rest relies on that line. The line approximates the value of ln(x) in the area near to x = 1. According to your line, any value of ln(1 + d) is going to be close to the value on the tangent line, in this case when x = 1 + d, the y value will be y = (1 + d) - 1 = d.

Bawx said:
2. Use the approximation from the previous part to deduce that

p = p(h) '=' Ae^-0.004h/30
What's p?

-Dan
 
This same problem was recently posted by another member, and you may find the discussion helpful:

http://mathhelpboards.com/calculus-10/y-ln-x-10679.html
 
Oh ok, so since ln(x) '=' x-1 you can just sub (1+d) to both sides?

Ah oops, I forgot to add the explanation above the questions:

Air pressure decays approximately exponentially at about 0.4 per cent for each rise of 30 metres above sea level. If we let p = p(h) denote air pressure (measured in some appropriate units) at h metres above sea level, then we can model this phenomenon using the equation

p = p(h) = Ae^kh

for some appropriate constants A and k.
 
MarkFL said:
This same problem was recently posted by another member, and you may find the discussion helpful:

http://mathhelpboards.com/calculus-10/y-ln-x-10679.html

Oh oops, I didn't realize that. Thanks for pointing it out! That one seems to get stuck on finding the tangent line tough, I hope it's ok if I keep using this thread. Sorry about that.
 
Bawx said:
Oh oops, I didn't realize that. Thanks for pointing it out! That one seems to get stuck on finding the tangent line tough, I hope it's ok if I keep using this thread. Sorry about that.

There's nothing wrong with posting a problem that has been posted before (it happens from time to time, we only discourage the same person from posting a problem more than once), I just wanted you to be able to see the discussion there as well. :D
 
If You can demonstrate that is...

$\displaystyle \lim_{d \rightarrow 0} \frac{\ln (1 + d)}{d} = 1\ (1)$

... then You can say that for 'small d' is $\displaystyle \ln (1 + d) \sim d$. The (1) is easily demonstrable using the concept of derivative but let's suppose You don't have yet such a concept and the only You know is the definition of exponential...

$\displaystyle e^{x} = \lim_{n \rightarrow \infty} (1 + \frac{x}{n})^{n}\ (2)$

... and the fact that logarithm is the inverse of exponential. What You can do is to compute the limit...

$\displaystyle \lim_{d \rightarrow 0} e^{\frac{\ln (1+d)}{d}} = \lim_{d \rightarrow 0} (1+ d)^{\frac{1}{d}} = \lim_{n \rightarrow \infty} (1+ \frac{1}{n})^{n} = e\ (3)$

... and (1) is demonstrated...

Kind regards

$\chi$ $\sigma$
 

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