Infinitesimal Definition and 143 Threads

In mathematics, an infinitesimal or infinitesimal number is a quantity that is closer to zero than any standard real number, but that is not zero. The word infinitesimal comes from a 17th-century Modern Latin coinage infinitesimus, which originally referred to the "infinity-th" item in a sequence.
Infinitesimals do not exist in the standard real number system, but they do exist in other number systems, such as the surreal number system and the hyperreal number system, which can be thought of as the real numbers augmented with both infinitesimal and infinite quantities; the augmentations are the reciprocals of one another.
Infinitesimal numbers were introduced in the development of calculus, in which the derivative was first conceived as a ratio of two infinitesimal quantities. This definition was not rigorously formalized. As calculus developed further, infinitesimals were replaced by limits, which can be calculated using the standard real numbers.
Infinitesimals regained popularity in the 20th century with Abraham Robinson's development of nonstandard analysis and the hyperreal numbers, which, after centuries of controversy, showed that a formal treatment of infinitesimal calculus was possible. Following this, mathematicians developed surreal numbers, a related formalization of infinite and infinitesimal numbers that includes both hyperreal numbers and ordinal numbers, which is the largest ordered field.
The insight with exploiting infinitesimals was that entities could still retain certain specific properties, such as angle or slope, even though these entities were infinitely small.Infinitesimals are a basic ingredient in calculus as developed by Leibniz, including the law of continuity and the transcendental law of homogeneity. In common speech, an infinitesimal object is an object that is smaller than any feasible measurement, but not zero in size—or, so small that it cannot be distinguished from zero by any available means. Hence, when used as an adjective in mathematics, infinitesimal means infinitely small, smaller than any standard real number. Infinitesimals are often compared to other infinitesimals of similar size, as in examining the derivative of a function. An infinite number infinitesimals are summed to calculate an integral.
The concept of infinitesimals was originally introduced around 1670 by either Nicolaus Mercator or Gottfried Wilhelm Leibniz. Archimedes used what eventually came to be known as the method of indivisibles in his work The Method of Mechanical Theorems to find areas of regions and volumes of solids. In his formal published treatises, Archimedes solved the same problem using the method of exhaustion. The 15th century saw the work of Nicholas of Cusa, further developed in the 17th century by Johannes Kepler, in particular calculation of area of a circle by representing the latter as an infinite-sided polygon. Simon Stevin's work on decimal representation of all numbers in the 16th century prepared the ground for the real continuum. Bonaventura Cavalieri's method of indivisibles led to an extension of the results of the classical authors. The method of indivisibles related to geometrical figures as being composed of entities of codimension 1. John Wallis's infinitesimals differed from indivisibles in that he would decompose geometrical figures into infinitely thin building blocks of the same dimension as the figure, preparing the ground for general methods of the integral calculus. He exploited an infinitesimal denoted 1/∞ in area calculations.
The use of infinitesimals by Leibniz relied upon heuristic principles, such as the law of continuity: what succeeds for the finite numbers succeeds also for the infinite numbers and vice versa; and the transcendental law of homogeneity that specifies procedures for replacing expressions involving inassignable quantities, by expressions involving only assignable ones. The 18th century saw routine use of infinitesimals by mathematicians such as Leonhard Euler and Joseph-Louis Lagrange. Augustin-Louis Cauchy exploited infinitesimals both in defining continuity in his Cours d'Analyse, and in defining an early form of a Dirac delta function. As Cantor and Dedekind were developing more abstract versions of Stevin's continuum, Paul du Bois-Reymond wrote a series of papers on infinitesimal-enriched continua based on growth rates of functions. Du Bois-Reymond's work inspired both Émile Borel and Thoralf Skolem. Borel explicitly linked du Bois-Reymond's work to Cauchy's work on rates of growth of infinitesimals. Skolem developed the first non-standard models of arithmetic in 1934. A mathematical implementation of both the law of continuity and infinitesimals was achieved by Abraham Robinson in 1961, who developed nonstandard analysis based on earlier work by Edwin Hewitt in 1948 and Jerzy Łoś in 1955. The hyperreals implement an infinitesimal-enriched continuum and the transfer principle implements Leibniz's law of continuity. The standard part function implements Fermat's adequality.
Vladimir Arnold wrote in 1990:

Nowadays, when teaching analysis, it is not very popular to talk about infinitesimal quantities. Consequently present-day students are not fully in command of this language. Nevertheless, it is still necessary to have command of it.

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  1. S

    Investigations into the infinitesimal Lorentz transformation

    Homework Statement [/B] A Lorentz transformation ##x^{\mu} \rightarrow x'^{\mu} = {\Lambda^{\mu}}_{\nu}x^{\nu}## is such that it preserves the Minkowski metric ##\eta_{\mu\nu}##, meaning that ##\eta_{\mu\nu}x^{\mu}x^{\nu}=\eta_{\mu\nu}x'^{\mu}x'^{\nu}## for all ##x##. Show that this implies...
  2. B

    I Can a Cat Catch a Mouse Running in a Circle at the Same Speed?

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  3. ytht100

    How to Calculate d(theta0)/d(theta1) in Snell's Law?

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  4. ShayanJ

    Lagrangian invariance under infinitesimal transformations

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  5. G

    Is this expression infinitesimal, finite, or infinite

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  6. M

    Are infinitesimal field variations in QFT similar to coordinate components?

    Hello, In the context of QFT, I do not understand the statement: ##\frac{\delta \phi(x)}{\delta \phi(y)}=\delta (x-y)## I understand the proof which arises from the definition of the functional derivative but I do not get its meaning. From what I see is generalizes ##\frac{\partial...
  7. M

    QFT: Lorentz Trans+ Field infinitesimal variation

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  8. C

    Infinitesimal conformal transformations

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  9. M

    Infinitesimal transformation of a field

    Hi, Could you please explain me why, under the transformation of a complex valued field Φ→eiαΦ, for an infinitesimal transformation we have the following relation? δΦ=iαΦ Thanks a lot
  10. Msilva

    Find infinitesimal displacement in any coordinate system

    I am wondering how can I find the infinitesimal displacement in any coordinate system. For example, in spherical coordinates we have the folow relations: x = \, \rho sin\theta cos\phi y = \, \rho sin\theta sin\phi z = \, \rho cos\theta And we have that d\vec l = dr\hat r +rd\theta\hat \theta...
  11. S

    Integral with symmetric infinitesimal bounds

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  12. TheDemx27

    How do you Treat Infinitesimals?

    All throughout calculus texts, the authors have always put conditions on the manipulation of differentials. They say that for the chain rule, the cancellation of the differentials is simply a way to remember the formula. When doing separation of variable for ODEs, texts always say something...
  13. j3dwards

    Infinitesimal Electric field of slice of disk

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  14. Vinay080

    What is the Euler's stand on infinitesimals?

    Euler was the master in analysisng anything. This can be seen in his words in the preface of his book "Mmathematica" (translated by Ian Bruce), where he speaks on the text of Hermann "Phoronomiam": Euler has given many insightful words on analysisng things in his preface of many other books...
  15. D

    Confused about using the integral and infinitesimal?

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  16. D

    Showing infinitesimal transformation is canonical

    Homework Statement So we have infinitesimal transformations from ##q_i## to ##\bar{q_i}## and ##p_i## to ##\bar{p_i}## ( where ##p_i## represents the canonical momentum conjugate of ##q_i##) given by $$\bar{q_i} = q_i + \epsilon \frac{\partial g}{\partial p_i}$$ $$\bar{p_i} = p_i - \epsilon...
  17. C

    Definition of derivative - infinitesimal approach, help :)

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  18. W

    Orthogonality from infinitesimal small rotation

    Hello buddies, Could someone please help me to understand where the second and the third equalities came from? Thanks,
  19. PWiz

    Infinitesimal displacement in spherical coordinates

    I'm trying to derive what ##ds^2## equals to in spherical coordinates. In Euclidean space, $$ds^2= dx^2+dy^2+dz^2$$ Where ##x=r \ cos\theta \ sin\phi## , ##y=r \ sin\theta \ sin\phi## , ##z=r \ cos\phi## (I'm using ##\phi## for the polar angle) For simplicity, let ##cos...
  20. D

    How Does the Wavefunction Propagate for Infinitesimal Times?

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  21. ognik

    Derive infinitesimal rotation operator

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  22. JonnyMaddox

    Infinitesimal transformations and Poisson brackets

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  23. P

    Understanding Infinitesimal Transformations in Rotational Symmetry

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  24. Ravi Mohan

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  25. C

    Rigorous Definition of Infinitesimal Projection Operator?

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  26. J

    Integral with infinitesimal under root

    I want compute the following integral: $$\\ \int f(x,y) \sqrt{dx^2+dy^2}$$ Is correct this pass-by-pass: $$\\ \sqrt{\left( \int f(x,y) \right)^2} \sqrt{dx^2+dy^2} = \sqrt{\left( \int f(x,y) \right)^2 (dx^2+dy^2)} = \sqrt{\left( \int f(x,y) \right)^2 dx^2 + \left( \int f(x,y) \right)^2 dy^2}...
  27. JonnyMaddox

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  28. J

    Dx as change in distance vs dx as infinitesimal x?

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  29. M

    Why do infinitesimal rotations commute but finite rotations do not?

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  30. T

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  31. J

    How Do Line and Surface Infinitesimals Differ in Mathematical Formulations?

    I think you know definition of line infinitesimal: [ds]^2 = \begin{bmatrix} dx & dy & dz \end{bmatrix} \begin{bmatrix} 1 & 0 & 0\\ 0 & 1 & 0\\ 0 & 0 & 1\\ \end{bmatrix}^2 \begin{bmatrix} dx\\ dy\\ dz\\ \end{bmatrix} = \begin{bmatrix} dr & d\theta & dz \end{bmatrix} \begin{bmatrix} 1 & 0 & 0\\ 0...
  32. G

    Infinitesimal volume using differentials

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  33. K

    Infinitesimal SUSY transformation of SYM lagrangian

    I tried to verify that the SYM lagrangian is invariant under SUSY transformation, but it turned out there is a term that doesn't vanish. The SYM lagrangian is: \mathscr{L}_{SYM}=-\frac{1}{4}F^{a\mu\nu}F^a_{\mu\nu}+i\lambda^{\dagger a}\bar{\sigma}^\mu D_\mu \lambda^a+\frac{1}{2}D^a D^a the...
  34. J

    When does infinitesimal notation break down?

    Everything I've encountered in physics so far allows infinitesimal numbers to be manipulated as real numbers. But there has been much criticism towards Leibniz's notation, and I assume it is for a reason. When in mathematics will the infinitesimal notation not work? Including treating...
  35. fluidistic

    Infinitesimal Lorentz transform and its inverse, tensors

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  36. S

    What's the deal on infinitesimal operators?

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  37. Y

    Angular momentum operators as infinitesimal generators

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  38. L

    Infinitesimal Canonical Transformation

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  39. A

    Rigorous treatment of infinitesimal reparametrizations

    Hi! Reading some string theory books I always find that the introductory chapters discuss the relativistic free particle (see Lüst-Theisen, or Becker-Becker-Schwarz, page 21, exercise 2.3). Then they go on about showing that the action S=-m\int^{t_1}_{t_2} dx = -m...
  40. R

    Infinitesimal generators of bridged stochastic process

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  41. S

    Why Can't We Calculate Sphere Surface Area with Infinitesimal Cylinders?

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  42. M

    Preservation of the infinitesimal element of length

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  43. B3NR4Y

    Superstring Theory problem. Infinitesimal supersymmetry transofrmations

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  44. J

    Write the expression for the infinitesimal radial inertal force dfr look at pic

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  45. N

    Applying Reynold's Theorem to Infinitesimal Element: Fluid Dynamics

    So Reynold's transport theorem states that \frac{\mathrm d}{\mathrm d t} \int_{V(t)} f \; \mathrm d V = \int_{V(t)} \partial_t f \; \mathrm d V + \int_{V(t)} \nabla \cdot \left( f \mathbf v \right) \; \mathrm d V. Now I would expect (on basis of conceptual reasoning) that if I were to apply...
  46. P

    Conformal group, infinitesimal transformation

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  47. pellman

    How are 1-forms related to infinitesimal displacements?

    Consider a point p in a manifold with coordinates x^\alpha and another point nearby with coordinates x^\alpha + dx^\alpha where dx are infinitesimal or arbitrarily small. Suppose we have a function f on this manifold. Then we can write df=f(x^\alpha + dx^\alpha)-f(x^\alpha)=\partial_\mu f...
  48. J

    Heat transferred during an infinitesimal quasi static process of an ideal gas

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  49. N

    How to calculate the order of an infinitesimal

    I know how to find out if an infinitesimal delta is of the first order (if delta*y/delta*x=dy/dx+epsilon is approximately equal to (dy/dx)*delta*x, but how do you find out if an infinitesimal is of second order or higher and how do you find out what that order is? Note: I will update this...
  50. W

    How can we achieve infinitesimal temperature difference during heat transfer

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