Does dx have mulitple personalites?

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The discussion centers on the interpretation of the differential notation "dx" in calculus, particularly its role in integration and differentiation. Participants clarify that "dx" represents an infinitesimally small quantity and can be viewed as a 1-form in advanced mathematics. The conversation also touches on the manipulation of differentials in ordinary differential equations (ODEs), emphasizing the importance of understanding the context in which "dx" is used. Ultimately, "dx" serves multiple purposes, including indicating the variable of integration and functioning as a measure.

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  • Understanding of basic calculus concepts, including integration and differentiation.
  • Familiarity with ordinary differential equations (ODEs) and their notation.
  • Knowledge of Riemann sums and their relationship to integrals.
  • Basic concepts of differential geometry, specifically 1-forms.
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  • Study the concept of 1-forms in differential geometry.
  • Learn about the Riemann integral and its formal definition.
  • Explore the manipulation of differentials in the context of ODEs.
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Mathematics students, educators, and anyone interested in deepening their understanding of calculus, particularly the nuances of differential notation and its applications in integration and ODEs.

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Can someone, who really knows and understands, tell me what dx (or whatever variables given) means behind the integral sign? I have seen more disagreement in Calculus books concerning this. Some authors say it's there just to "indicate the variable" your integrating with respect to, i.e., its not formally required. I had a mathematics professor tell me otherwise, namely that dx is a "real" variable and is required, multiplying at every point with f(x), defining a virtual infinite number of Reimannian rectangles as in S f(x)dx, (S means sum) and performing the normal integration.

Also, (and this ties in) if I have for example, a simple separable ODE such as:

m dv/dt = mg -kv

(where g is accelleration due to gravity, m is mass, v is velocity and k is frictional constant), and if we assume dv/dt is the standard Leibniz operator notation for a derivative, then how can one simply multiply dt through, when it's actually part of an operator? Now I have read that by "appropriately" defining dt, then defining dv as dv = v' dt, we get of course v' = dv/dt. Now, having defined dv/dt as a ratio of differentials, using the same Leibniz notation, we should NOW be able to use basic algebraic techniques with little worry. But wait, if we now integrate both sides:

S (1/(g - cv))dv = S dt where S means sum, and c = k/m,

I still don't know how to interpret S dt? Or now S (1/g-cv)dv for that matter? Do I sound confused? I am! Any help on this is greatly appreciated. I need to understand this.
 
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Yes

dx does indeed have "multiple personalities".


The intuition is that dx is "supposed" to be an "infinitessimally small quantity". The notation for many concepts in analysis was specifically chosen so that it looked like you really were manipulating infinitessimally small quantities.



Am I presuming correctly that when you write

(1/g - cv)

You mean

\frac{1}{g - cv}

? If so, you wrote it wrong; you need to wrap the denominator in parentheses, such as: (1 / (g - cv))


Anyways:

\int \frac{dv}{g - cv}

is certainly in the form you mentioned earlier. If we write f(z) = 1 / (g - cz), then we have:

\int \frac{dv}{g - cv} = \int f(v) \, dv

so you can use your favorite intuitive interpretation of \int f(x)\,dx to interpret this integral.
 
The entity dx is really something called a "1-form." You can feed a vector field v to a 1-form \omega, and it spits out a real-valued function \omega(v).

In more precise terms, a 1-form on a manifold M is a map from \text{Vect}(M) to C^\infty(M) that is linear over C^\infty(M). \text{Vect}(M) is the set of all vector fields that can be defined on M, and C^\infty(M) is the set of all smooth (real-valued) functions on M.

So, really, the differential dx has only one real personality -- that of a 1-form. Much of this formality is not needed in basic calculus classes, however, and this 1-form can be somewhat abused so that it appears to take on other roles, particularly in flat spaces.

- Warren
 
in addition to being a 1-form, i was going to mention that dx is also a measure, which is a totally different kind of gadget.

i would say, yeah, it definitely has multiple personalities.
 
Originally posted by lethe
in addition to being a 1-form, i was going to mention that dx is also a measure, which is a totally different kind of gadget.

Yeah, I forgot about that.. hehe... suppose you're right, it's an entity that can function as anyone of a handful of mathematical devices.

- Warren
 


Originally posted by Hurkyl
dx does indeed have "multiple personalities".


The intuition is that dx is "supposed" to be an "infinitessimally small quantity". The notation for many concepts in analysis was specifically chosen so that it looked like you really were manipulating infinitessimally small quantities.



Am I presuming correctly that when you write



You mean

\frac{1}{g - cv}

? If so, you wrote it wrong; you need to wrap the denominator in parentheses, such as: (1 / (g - cv))


Anyways:

\int \frac{dv}{g - cv}

is certainly in the form you mentioned earlier. If we write f(z) = 1 / (g - cz), then we have:

\int \frac{dv}{g - cv} = \int f(v) \, dv

so you can use your favorite intuitive interpretation of \int f(x)\,dx to interpret this integral.

Sorry about the parentheses; I corrected it. Actually, I want to know what dx represents behind the integral sign.

Why is it needed, other than to indicate the variable your integrating with respect to? In my calculus book, the first time dx shows up behind the integral, is in the definition of an integral as the limit of a Reimann sum. But my author indicates that dx in that context is not to be confused with dx as it applies to a derivative. I find that hard to believe. But because I'm not a mathematician, for now, I'm going to assume I don't understand. He mentions it's there only for convenience, and useful for such purposes as u du substitution. Once I understand this, I think manipulation of dx in a DE will make sense. In the ODE example, dx is part of a derivative one second, then (by simple multiplcation) behind the integral in the next. Does dx mean the same thing in both cases? I know it's required for a derivative, but what about the integral? What do you think?
 
Does this manipulation make it easier to digest?

<br /> m v&#039;(t) = mg - kv(t)<br />
<br /> \frac{1}{g - c v(t)} v&#039;(t) = 1<br />
<br /> \int \frac{1}{g - c v(t)} v&#039;(t) \, dt = \int 1 \, dt<br />

By substitution, we know

<br /> \int \frac{1}{g - c u} \, du = \int \frac{1}{g - c v(t)} v&#039;(t) \, dt<br />

Which let's us finish off the problem.
 
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