Pagine


Visualizzazione post con etichetta Measurement. Mostra tutti i post
Visualizzazione post con etichetta Measurement. Mostra tutti i post

sabato 22 gennaio 2011

The search of a straight-line mechanism

During the centuries, the problem to describe a straight line was one that tickled the fancies of mathematicians, of ingenious mechanics, and of gentlemanly dabblers in ideas. Sir Alfred Bray Kempe was a mathematician  who discovered (in 1877) new straight line linkages and published his influential lectures on the subject.


You can read his theories in the book "How to draw a straight line" available on line by clicking here

sabato 13 novembre 2010

Straight and curved in "scientific" stamps



These are some stamps related to various branches of science.
On them are depicted straight lines, curves and spirals typical
of the world of mathemayics, physics and chemistry.

Two mathematicians and their curves on stamps



Gottfried Wilhelm von Leibniz (1646-1716): mathematician, scientist, philosopher.
Coins the term "function": it is necessary to identify the various quantities associated to a curve, including its value, the slope and the perpendicular at one point.

Friedrich Wilhelm Bessel (1784-1846): mathematician, astronomer.
He was the first to determine the distance of a star by measuring the parallax of 61 Cygni in 1838. With his precise observations could categorize the locations of more than 50000 stars and then he introduced mathematical functions now know by his name.

mercoledì 10 novembre 2010

Simple harmonic motion



In physics, simple harmonic motion (SHM) is a periodic motion that is neither driven nor damped. An object in simple harmonic motion experiences a net force which obeys Hooke's law; that is, the force is directly proportional to the displacement from the equilibriliium position and acts in the opposite direction of the displacement.
A simple harmonic oscilattor is a system which undergoes simple harmonic motion. The oscillator oscillates about an equilibrium position (or mean position) between two extreme positions of maximum displacement in a periodic manner. In fact, the motion of the oscillator can be described by means of a sinusoidal function. Mathematically, the displacement from the equilibrium position x is given by
 x(t) = A\cos\left(\omega t + \phi\right),
where
A is the amplitude which is the maximum distance from the equilibrium position (in SI units m);
ω is the angular frequency which is a multiple of frequency f, and ω = 2πf (in SI unit: s-1);
φ is the phasewhich is the elapsed fraction of wave cycle.
http://en.wikipedia.org/wiki/Simple_harmonic_motion

mercoledì 3 novembre 2010

Straight and Curved: measuring and drawing tools



Some useful tools to measure and draw straight and curved line

A body falls straight or ...?


Guglielmini experiment
It showed that a body dropped from a height not have
a rectilinear motion because the Earth's rotation


Foucault pendulum: a straight cable to measure a rotation



The Foucault pendulum (1870) made it possible to demonstrate for the first time directly the phenomenon of Earth's rotation. It is a sphere of lead covered with iron and it suspended from the ceiling by a long steel cable that is put into oscillation to demonstrate the phenomenon of Earth's rotation.

giovedì 21 ottobre 2010

Measurement


In mathematics, curvature refers to any of a number of loosely related concepts in different areas of geometry. Intuitively, curvature is the amount by which a geometric object deviates from being flat, or straight in the case of a line, but this is defined in different ways depending on the context. There is a key distinction between extrinsic curvature, which is defined for objects embedded in another space (usually a Euclidean space) in a way that relates to the radius of curvature of circles that touch the object, and intrinsic curvature, which is defined at each point in aRiemannian manifold. This article deals primarily with the first concept.
The canonical example of extrinsic curvature is that of a circle, which everywhere has curvature equal to the reciprocal of its radius.

For a plane curve C, the mathematical definition of curvature uses a parametric representation of C with respect to the arc length parametrization. It can be computed given any regular parametrization by a more complicated formula given below.
Let γ(s) be a regular parametric curve, where s is the arc length, or natural parameter. This determines the unit tangent vector T(s), the unit normal vector N(s), the curvature κ(s), the oriented or signed curvature k(s), and the radius of curvature R(s) at each point:



The curvature of a straight line is identically zero. The curvature of a circle of radius R is constant, i.e. it does not depend on the point and is equal to the reciprocal of the radius:



Thus for a circle, the radius of curvature is simply its radius. Straight lines and circles are the only plane curves whose curvature is constant. Given any curve C and a point P on it where the curvature is non-zero, there is a unique circle which most closely approximates the curve near P, the osculating circle at P. The radius of the osculating circle is the radius of curvature of C at this point.