"The integral along two different paths will always have the same value if it is never the case that φ(x) = ∞ in the space between the curves representing the paths. This is a beautiful theorem, whose not-too-difficult proof I will give at a suitable opportunity." (Carl F Gauss, [letter to Bessel] 1811)
"The integral ∫ϕx.dx will always have the same value along two different paths if it is never the case that ϕx = ∞ in the space between the curves representing the paths. This is abeautiful theorem whose not-too-difficult proof I will give at a suitable opportunity [. . . ]. In any case this makes it immediately clear why a function arising from an integral ϕx.dx can have many values for a single value of x, for one can go round a point where ϕx = ∞ either not at all, or once, or several times. For example, if one defines logx by dx x , starting from x = 1, one comes to logx either without enclosing the point x = 0 or by going around it once or several times; each time the constant +2πi or −2πi enters; so the multiple of logarithms of any number are quite clear." (Carl FriedrichGauss, [letter to Bessel] 1821)
"The effects of heat are subject to constant laws which cannot be discovered without the aid of mathematical analysis. The object of the theory is to demonstrate these laws; it reduces all physical researches on the propagation of heat, to problems of the integral calculus, whose elements are given by experiment. No subject has more extensive relations with the progress of industry and the natural sciences; for the action of heat is always present, it influences the processes of the arts, and occurs in all the phenomena of the universe." (Jean-Baptiste-Joseph Fourier, "The Analytical Theory of Heat", 1822)
"The integrals which we have obtained are not only general expressions which satisfy the differential equation, they represent in the most distinct manner the natural effect which is the object of the phenomenon [...] when this condition is fulfilled, the integral is, properly speaking, the equation of the phenomenon; it expresses clearly the character and progress of it, in the same manner as the finite equation of a line or curved surface makes known all the properties of those forms." (Jean-Baptiste-Joseph Fourier, "Théorie Analytique de la Chaleur", 1822)
"I have throughout introduced the Integral Calculus in connexion with the Differential Calculus [...] Is it always proper to learn every branch of a direct subject before anything connected with the inverse relation is considered? If so why are not multiplication and involution in arithmetic made to follow addition and precede subtraction? The portion of the Integral Calculus, which properly belongs to any given portion of the Differential Calculus increases its power a hundred-fold [...]" (Augustus De Morgan, "The Differential and Integral Calculus", 1836)
"A definite Integral always presupposes numeric values; consequently equations in which definite integrals occur are seldom or never correct as general (formal) equations, but can only be admitted as numeric equations; consequently the convergence of any infinite series which may occur in them is an indispensable condition, whereas the condition of convergence with respect to a general series in general investigations, such as must be necessarily first established as the foundation of the possibility of any calculation, is quite as absurd [...]" (Martin Ohm, "The Spirit of Mathematical Analysis and its Relation to a Logical System", 1842)
"Therefore one has taken everywhere the opposite road, and each time one encounters manifolds of several dimensions in geometry, as in the doctrine of definite integrals in the theory of imaginary quantities, one takes spatial intuition as an aid. It is well known how one gets thus a real overview over the subject and how only thus are precisely the essential points emphasized." (Bernhard Riemann)
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