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<title>The Notebooks of Leonardo Da Vinci</title>
<link>http://interconnected.org/home/more/davinci/</link>
<description>Day-by-day Da Vinci. Read the pages of the Notebooks by RSS, one at a time. This feed began on 15 May 2008.</description>

<item>
<title>Page 86</title>
<link>http://interconnected.org/home/more/davinci/86.html</link>
<description><![CDATA[<p>A simple and natural method; showing how objects appear to the eye
<br>without any other medium.
<br>
<br>The object that is nearest to the eye always seems larger than
<br>another of the same size at greater distance. The eye _m_, seeing
<br>the spaces _o v x_, hardly detects the difference between them, and
<br>the. reason of this is that it is close to them [Footnote 6: It is
<br>quite inconceivable to me why M. RAVAISSON, in a note to his French
<br>translation of this simple passage should have remarked: _Il est
<br>clair que c'est par erreur que Leonard a ecrit_ per esser visino _au
<br>lieu de_ per non esser visino. (See his printed ed. of MS. A. p.
<br>38.)]; but if these spaces are marked on the vertical plane _n o_
<br>the space _o v_ will be seen at _o r_, and in the same way the space
<br>_v x_ will appear at _r q_. And if you carry this out in any place
<br>where you can walk round, it will look out of proportion by reason
<br>of the great difference in the spaces _o r_ and _r q_. And this
<br>proceeds from the eye being so much below [near] the plane that the
<br>plane is foreshortened. Hence, if you wanted to carry it out, you
<br>would have [to arrange] to see the perspective through a single hole
<br>which must be at the point _m_, or else you must go to a distance of
<br>at least 3 times the height of the object you see. The plane _o p_
<br>being always equally remote from the eye will reproduce the objects
<br>in a satisfactory way, so that they may be seen from place to place.</p>]]></description>
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<item>
<title>Page 85</title>
<link>http://interconnected.org/home/more/davinci/85.html</link>
<description><![CDATA[<p>PERSPECTIVE.
<br>
<br>The vertical plane is a perpendicular line, imagined as in front of
<br>the central point where the apex of the pyramids converge. And this
<br>plane bears the same relation to this point as a plane of glass
<br>would, through which you might see the various objects and draw them
<br>on it. And the objects thus drawn would be smaller than the
<br>originals, in proportion as the distance between the glass and the
<br>eye was smaller than that between the glass and the objects.
<br>
<br>PERSPECTIVE.
<br>
<br>The different converging pyramids produced by the objects, will
<br>show, on the plane, the various sizes and remoteness of the objects
<br>causing them.
<br>
<br>PERSPECTIVE.
<br>
<br>All those horizontal planes of which the extremes are met by
<br>perpendicular lines forming right angles, if they are of equal width
<br>the more they rise to the level of eye the less this is seen, and
<br>the more the eye is above them the more will their real width be
<br>seen.
<br>
<br>PERSPECTIVE.
<br>
<br>The farther a spherical body is from the eye the more you will see
<br>of it.
<br>
<br>The angle of sight varies with the distance (86-88)</p>]]></description>
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<item>
<title>Page 84</title>
<link>http://interconnected.org/home/more/davinci/84.html</link>
<description><![CDATA[<p>Pictorial perspective can never make an object at the same distance,
<br>look of the same size as it appears to the eye. You see that the
<br>apex of the pyramid _f c d_ is as far from the object _c_ _d_ as the
<br>same point _f_ is from the object _a_ _b_; and yet _c_ _d_, which is
<br>the base made by the painter's point, is smaller than _a_ _b_ which
<br>is the base of the lines from the objects converging in the eye and
<br>refracted at _s_ _t_, the surface of the eye. This may be proved by
<br>experiment, by the lines of vision and then by the lines of the
<br>painter's plumbline by cutting the real lines of vision on one and
<br>the same plane and measuring on it one and the same object.</p>]]></description>
</item>

<item>
<title>Page 83</title>
<link>http://interconnected.org/home/more/davinci/83.html</link>
<description><![CDATA[<p>OF THE PLANE OF GLASS.
<br>
<br>Perspective is nothing else than seeing place [or objects] behind a
<br>plane of glass, quite transparent, on the surface of which the
<br>objects behind that glass are to be drawn. These can be traced in
<br>pyramids to the point in the eye, and these pyramids are intersected
<br>on the glass plane.</p>]]></description>
</item>

<item>
<title>Page 82</title>
<link>http://interconnected.org/home/more/davinci/82.html</link>
<description><![CDATA[<p>An experiment showing that though the pupil may not be moved from
<br>its position the objects seen by it may appear to move from their
<br>places.
<br>
<br>If you look at an object at some distance from you and which is
<br>below the eye, and fix both your eyes upon it and with one hand
<br>firmly hold the upper lid open while with the other you push up the
<br>under lid--still keeping your eyes fixed on the object gazed at--you
<br>will see that object double; one [image] remaining steady, and the
<br>other moving in a contrary direction to the pressure of your finger
<br>on the lower eyelid. How false the opinion is of those who say that
<br>this happens because the pupil of the eye is displaced from its
<br>position.
<br>
<br>How the above mentioned facts prove that the pupil acts upside down
<br>in seeing.
<br>
<br>[Footnote: 82. 14--17. The subject indicated by these two headings is
<br>fully discussed in the two chapters that follow them in the
<br>original; but it did not seem to me appropriate to include them
<br>here.]
<br>
<br>Demostration of perspective by means of a vertical glass plane
<br>(83-85).</p>]]></description>
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<item>
<title>Page 81</title>
<link>http://interconnected.org/home/more/davinci/81.html</link>
<description><![CDATA[<p>HOW THE INNUMERABLE RAYS FROM INNUMERABLE IMAGES CAN CONVERGE TO A
<br>POINT.
<br>
<br>Just as all lines can meet at a point without interfering with each
<br>other--being without breadth or thickness--in the same way all the
<br>images of surfaces can meet there; and as each given point faces the
<br>object opposite to it and each object faces an opposite point, the
<br>converging rays of the image can pass through the point and diverge
<br>again beyond it to reproduce and re-magnify the real size of that
<br>image. But their impressions will appear reversed--as is shown in
<br>the first, above; where it is said that every image intersects as it
<br>enters the narrow openings made in a very thin substance.
<br>
<br>Read the marginal text on the other side.
<br>
<br>In proportion as the opening is smaller than the shaded body, so
<br>much less will the images transmitted through this opening intersect
<br>each other. The sides of images which pass through openings into a
<br>dark room intersect at a point which is nearer to the opening in
<br>proportion as the opening is narrower. To prove this let _a b_ be an
<br>object in light and shade which sends not its shadow but the image
<br>of its darkened form through the opening _d e_ which is as wide as
<br>this shaded body; and its sides _a b_, being straight lines (as has
<br>been proved) must intersect between the shaded object and the
<br>opening; but nearer to the opening in proportion as it is smaller
<br>than the object in shade. As is shown, on your right hand and your
<br>left hand, in the two diagrams _a_ _b_ _c_ _n_ _m_ _o_ where, the
<br>right opening _d_ _e_, being equal in width to the shaded object _a_
<br>_b_, the intersection of the sides of the said shaded object occurs
<br>half way between the opening and the shaded object at the point _c_.
<br>But this cannot happen in the left hand figure, the opening _o_
<br>being much smaller than the shaded object _n_ _m_.
<br>
<br>It is impossible that the images of objects should be seen between
<br>the objects and the openings through which the images of these
<br>bodies are admitted; and this is plain, because where the atmosphere
<br>is illuminated these images are not formed visibly.
<br>
<br>When the images are made double by mutually crossing each other they
<br>are invariably doubly as dark in tone. To prove this let _d_ _e_ _h_
<br>be such a doubling which although it is only seen within the space
<br>between the bodies in _b_ and _i_ this will not hinder its being
<br>seen from _f_ _g_ or from _f_ _m_; being composed of the images _a_
<br>_b_ _i_ _k_ which run together in _d_ _e_ _h_.
<br>
<br>[Footnote: 81. On the original diagram at the beginning of this
<br>chapter Leonardo has written "_azurro_" (blue) where in the
<br>facsimile I have marked _A_, and "_giallo_" (yellow) where _B_
<br>stands.]
<br>
<br>[Footnote: 15--23. These lines stand between the diagrams I and III.]
<br>
<br>[Footnote: 24--53. These lines stand between the diagrams I and II.]
<br>
<br>[Footnote: 54--97 are written along the left side of diagram I.]</p>]]></description>
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<item>
<title>Page 80</title>
<link>http://interconnected.org/home/more/davinci/80.html</link>
<description><![CDATA[<p>AS TO WHETHER THE CENTRAL LINE OF THE IMAGE CAN BE INTERSECTED, OR
<br>NOT, WITHIN THE OPENING.
<br>
<br>It is impossible that the line should intersect itself; that is,
<br>that its right should cross over to its left side, and so, its left
<br>side become its right side. Because such an intersection demands two
<br>lines, one from each side; for there can be no motion from right to
<br>left or from left to right in itself without such extension and
<br>thickness as admit of such motion. And if there is extension it is
<br>no longer a line but a surface, and we are investigating the
<br>properties of a line, and not of a surface. And as the line, having
<br>no centre of thickness cannot be divided, we must conclude that the
<br>line can have no sides to intersect each other. This is proved by
<br>the movement of the line _a f_ to _a b_ and of the line _e b_ to _e
<br>f_, which are the sides of the surface _a f e b_. But if you move
<br>the line _a b_ and the line _e f_, with the frontends _a e_, to the
<br>spot _c_, you will have moved the opposite ends _f b_ towards each
<br>other at the point _d_. And from the two lines you will have drawn
<br>the straight line _c d_ which cuts the middle of the intersection of
<br>these two lines at the point _n_ without any intersection. For, you
<br>imagine these two lines as having breadth, it is evident that by
<br>this motion the first will entirely cover the other--being equal
<br>with it--without any intersection, in the position _c d_. And this
<br>is sufficient to prove our proposition.</p>]]></description>
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<item>
<title>Page 79</title>
<link>http://interconnected.org/home/more/davinci/79.html</link>
<description><![CDATA[<p>OF THE CENTRAL LINE OF THE EYE.
<br>
<br>Only one line of the image, of all those that reach the visual
<br>virtue, has no intersection; and this has no sensible dimensions
<br>because it is a mathematical line which originates from a
<br>mathematical point, which has no dimensions.
<br>
<br>According to my adversary, necessity requires that the central line
<br>of every image that enters by small and narrow openings into a dark
<br>chamber shall be turned upside down, together with the images of the
<br>bodies that surround it.</p>]]></description>
</item>

<item>
<title>Page 78</title>
<link>http://interconnected.org/home/more/davinci/78.html</link>
<description><![CDATA[<p>Necessity has provided that all the images of objects in front of
<br>the eye shall intersect in two places. One of these intersections is
<br>in the pupil, the other in the crystalline lens; and if this were
<br>not the case the eye could not see so great a number of objects as
<br>it does. This can be proved, since all the lines which intersect do
<br>so in a point. Because nothing is seen of objects excepting their
<br>surface; and their edges are lines, in contradistinction to the
<br>definition of a surface. And each minute part of a line is equal to
<br>a point; for _smallest_ is said of that than which nothing can be
<br>smaller, and this definition is equivalent to the definition of the
<br>point. Hence it is possible for the whole circumference of a circle
<br>to transmit its image to the point of intersection, as is shown in
<br>the 4th of this which shows: all the smallest parts of the images
<br>cross each other without interfering with each other. These
<br>demonstrations are to illustrate the eye. No image, even of the
<br>smallest object, enters the eye without being turned upside down;
<br>but as it penetrates into the crystalline lens it is once more
<br>reversed and thus the image is restored to the same position within
<br>the eye as that of the object outside the eye.</p>]]></description>
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<item>
<title>Page 77</title>
<link>http://interconnected.org/home/more/davinci/77.html</link>
<description><![CDATA[<p>THE PRINCIPLE ON WHICH THE IMAGES OF BODIES PASS IN BETWEEN THE
<br>MARGINS OF THE OPENINGS BY WHICH THEY ENTER.
<br>
<br>What difference is there in the way in which images pass through
<br>narrow openings and through large openings, or in those which pass
<br>by the sides of shaded bodies? By moving the edges of the opening
<br>through which the images are admitted, the images of immovable
<br>objects are made to move. And this happens, as is shown in the 9th
<br>which demonstrates: [Footnote 11: _per la 9a che dicie_. When
<br>Leonardo refers thus to a number it serves to indicate marginal
<br>diagrams; this can in some instances be distinctly proved. The ninth
<br>sketch on the page W. L. 145 b corresponds to the middle sketch of
<br>the three reproduced.] the images of any object are all everywhere,
<br>and all in each part of the surrounding air. It follows that if one
<br>of the edges of the hole by which the images are admitted to a dark
<br>chamber is moved it cuts off those rays of the image that were in
<br>contact with it and gets nearer to other rays which previously were
<br>remote from it &c.
<br>
<br>OF THE MOVEMENT OF THE EDGE AT THE RIGHT OR LEFT, OR THE UPPER, OR
<br>LOWER EDGE.
<br>
<br>If you move the right side of the opening the image on the left will
<br>move [being that] of the object which entered on the right side of
<br>the opening; and the same result will happen with all the other
<br>sides of the opening. This can be proved by the 2nd of this which
<br>shows: all the rays which convey the images of objects through the
<br>air are straight lines. Hence, if the images of very large bodies
<br>have to pass through very small holes, and beyond these holes
<br>recover their large size, the lines must necessarily intersect.
<br>
<br>[Footnote: 77. 2. In the first of the three diagrams Leonardo had
<br>drawn only one of the two margins, et _m_.]</p>]]></description>
</item>

<item>
<title>Page 76</title>
<link>http://interconnected.org/home/more/davinci/76.html</link>
<description><![CDATA[<p>The inversion of the images.
<br>
<br>All the images of objects which pass through a window [glass pane]
<br>from the free outer air to the air confined within walls, are seen
<br>on the opposite side; and an object which moves in the outer air
<br>from east to west will seem in its shadow, on the wall which is
<br>lighted by this confined air, to have an opposite motion.</p>]]></description>
</item>

<item>
<title>Page 75</title>
<link>http://interconnected.org/home/more/davinci/75.html</link>
<description><![CDATA[<p>If the judgment of the eye is situated within it, the straight lines
<br>of the images are refracted on its surface because they pass through
<br>the rarer to the denser medium. If, when you are under water, you
<br>look at objects in the air you will see them out of their true
<br>place; and the same with objects under water seen from the air.
<br>
<br>The intersection of the rays (76-82).</p>]]></description>
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<item>
<title>Page 74</title>
<link>http://interconnected.org/home/more/davinci/74.html</link>
<description><![CDATA[<p>The lines sent forth by the image of an object to the eye do not
<br>reach the point within the eye in straight lines.</p>]]></description>
</item>

<item>
<title>Page 73</title>
<link>http://interconnected.org/home/more/davinci/73.html</link>
<description><![CDATA[<p>The object which is opposite to the pupil of the eye is seen by that
<br>pupil and that which is opposite to the eye is seen by the pupil.
<br>
<br>Refraction of the rays falling upon the eye (74. 75)</p>]]></description>
</item>

<item>
<title>Page 72</title>
<link>http://interconnected.org/home/more/davinci/72.html</link>
<description><![CDATA[<p>In the practice of perspective the same rules apply to light and to
<br>the eye.</p>]]></description>
</item>

<item>
<title>Page 71</title>
<link>http://interconnected.org/home/more/davinci/71.html</link>
<description><![CDATA[<p>HOW THE IMAGES OF OBJECTS RECEIVED BY THE EYE INTERSECT WITHIN THE
<br>CRYSTALLINE HUMOUR OF THE EYE.
<br>
<br>An experiment, showing how objects transmit their images or
<br>pictures, intersecting within the eye in the crystalline humour, is
<br>seen when by some small round hole penetrate the images of
<br>illuminated objects into a very dark chamber. Then, receive these
<br>images on a white paper placed within this dark room and rather near
<br>to the hole and you will see all the objects on the paper in their
<br>proper forms and colours, but much smaller; and they will be upside
<br>down by reason of that very intersection. These images being
<br>transmitted from a place illuminated by the sun will seem actually
<br>painted on this paper which must be extremely thin and looked at
<br>from behind. And let the little perforation be made in a very thin
<br>plate of iron. Let _a b e d e_ be the object illuminated by the sun
<br>and _o r_ the front of the dark chamber in which is the said hole at
<br>_n m_. Let _s t_ be the sheet of paper intercepting the rays of the
<br>images of these objects upside down, because the rays being
<br>straight, _a_ on the right hand becomes _k_ on the left, and _e_ on
<br>the left becomes _f_ on the right; and the same takes place inside
<br>the pupil.
<br>
<br>[Footnote: This chapter is already known through a translation into
<br>French by VENTURI. Compare his '_Essai sur les ouvrages
<br>physico-mathematiques de L. da Vinci avec des fragments tires de ses
<br>Manuscrits, apportes de l'Italie. Lu a la premiere classe de
<br>l'Institut national des Sciences et Arts.' Paris, An V_ (1797).]
<br>
<br>The practice of perspective (72. 73).</p>]]></description>
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