Dimensions in logarithms after integration

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Homework Help Overview

The discussion revolves around the integration of a velocity function defined as v = 1 / kt, where participants explore the implications of dimensional analysis in logarithmic expressions resulting from integration. The subject area includes calculus and physics, particularly focusing on the interpretation of integrals in the context of motion and dimensional consistency.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants examine the integration of the velocity function and question how the resulting logarithmic argument can be dimensioned. Some explore the implications of using initial conditions and the challenges posed by undefined values at t=0. Others discuss the necessity of definite integrals in physical contexts and the assumptions underlying the integration process.

Discussion Status

The discussion is ongoing, with participants raising various interpretations and concerns about the dimensionality of logarithmic arguments and the validity of indefinite versus definite integrals in physical scenarios. Some guidance has been offered regarding the need for clear initial conditions and the implications of undefined values, but no consensus has been reached.

Contextual Notes

Participants note that the integration process leads to undefined expressions at certain points, particularly at t=0, which complicates the establishment of initial conditions. There is also a recognition that physical interpretations of mathematical expressions require careful consideration of starting and ending points in the context of motion.

quantum13
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Homework Statement


Let v = 1 / kt

v = m/s
k = 1/m
t = s

v = dx/dt so dx = dt / kt

integrating,

x = ln (kt)/k + C

However the argument of a logarithm is dimensionless. But an integration is a perfectly normal thing to do. So how come this integration results in a dimensional logarithm argument?
 
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What is constant C? Doing it right gives you

x=\int^{t_1}_{t_2}\frac{dt}{kt}=\frac{1}{k}(ln(t_2)-ln(t_1))=\frac{1}{k}ln\left(\frac{t_2}{t_1}\right)

The argument of the natural log is dimensionless as it should be.
 
d'oh the summer makes me forget even how to do basic integrals

but what if you do the integral in a non-definite way and use the constant C turning it into an initial value problem

dx = dt / kt
x = ln(t) / k + C
and use t=0, x=x0

but with this way i get ln(0), so how do i figure out C?

i know I am making some mistake but i can't seem to figure it out..
 
I want to know v_{t=0}=?
in your model k!=constant!
 
quantum13 said:
d'oh the summer makes me forget even how to do basic integrals

but what if you do the integral in a non-definite way and use the constant C turning it into an initial value problem

dx = dt / kt
x = ln(t) / k + C
and use t=0, x=x0

but with this way i get ln(0), so how do i figure out C?

i know I am making some mistake but i can't seem to figure it out..

Your equation for velocity is undefined for t=0, so it's no surprise that the position is equally undefined there.

You can't solve it as an initial value problem because of the specific function. You end up with dimensions in the argument. You can't talk about a function f(t)=x of how much distance the particle has traveled since time t=0 because that specific integral diverges, so you must take the definite integral for f(t)=x and only speak of differences in this function for t>0

And since you can't take the definite integral of one side of the equation, and the indefinite integral of the other side, you must therefore take the definite integral of both.

For instance, if we define x(t=1) = x_0 as an initial condition, we avoid the whole thing about the function being undefined at our chosen initial value, but the function f(t)=x as specified by the indefinite integral is still poorly defined.

kx=\ln{t}+kC

(Note how in the next step, if we were to measure time in any other units, we would not receive \ln{1} but some other value!)

kx_0=\ln{1}+kC
C=x_0

x=\frac{kx_0+\ln{t}}{k}

Bringing both terms into the logarithm:
x=\frac{\ln{(e^{kx_0}\cdot t)}}{k}

And so our argument for the logarithm still has dimensions of time, which proves we made a serious mistake somewhere along the way.
 
quantum13 said:
but what if you do the integral in a non-definite way and use the constant C turning it into an initial value problem
...
In physics there are no indefinite integrals, if you think about it for a moment, because mathematical expressions model physical reality. To take a simpler case, suppose you want to solve v = dx/dt = constant, the simplest differential equation there is. You can immediately write the mathematical expression x = vt + C if you are doing "math". What does this mean physically?

Physically you would say, I know that the rate of change of position with respect to time is constant. To find the overall change of position I need to write its incremental change as

dx = v dt

and add all such increments. But how exactly are you going to add them? You need a starting and ending point for both position and time, so you say

\int^{x}_{x_0}dx=\int^{t}_{t_0}vdt

(x-x0)=v(t-t0)

The symbols represent the starting space-time point (x0, t0) and the ending space-time point (x, t) of the summation. When you write x = vt, the assumption is that (a) the clock that measures time starts when motion starts (t0=0) and (b) that the object is at the origin when the clock starts (x0=0). Just because they are swept under the rug does not mean that they are not or should not be there. To put it in a nutshell, any summation requires a starting and an ending point and if you really don't know what these are, then you cannot do the summation.
 
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