The Elements of Perspective: arranged for the use of schools and intended to be read in connection with the first three books of EuclidRuskin, John
Science
The Elements of Perspective: arranged for the use of schools and intended to be read in connection with the first three books of Euclid
Ruskin, John
Perspective
[30] As in algebraic science, much depends, in complicated
perspective, on the student’s ready invention of expedients,
and on his quick sight of the shortest way in which the
solution may be accomplished, when there are several ways.
[31] The greatest masters are also fond of parallel perspective,
that is to say, of having one side of their buildings fronting
them full, and therefore parallel to the picture plane, while
the other side vanishes to the sight-point. This is almost
always done in figure backgrounds, securing simple and balanced
lines.
APPENDIX.
I.
PRACTICE AND OBSERVATIONS.
II.
DEMONSTRATIONS.
I.
PRACTICE AND OBSERVATIONS ON THE PRECEDING PROBLEMS.
PROBLEM I.
An example will be necessary to make this problem clear to the general
student.
The nearest corner of a piece of pattern on the carpet is 4½ feet
beneath the eye, 2 feet to our right and 3½ feet in direct distance
from us. We intend to make a drawing of the pattern which shall be
seen properly when held 1½ foot from the eye. It is required to fix
the position of the corner of the piece of pattern.
[Illustration: Fig. 51.]
Let _AB_, Fig. 51., be our sheet of paper, some 3 feet wide. Make _ST_
equal to 1½ foot. Draw the line of sight through _S_. Produce _TS_,
and make _DS_ equal to 2 feet, therefore _TD_ equal to 3½ feet. Draw
_DC_, equal to 2 feet; _CP_, equal to 4 feet. Join _TC_ (cutting the
sight-line in _Q_) and _TP_.
Let fall the vertical _QP′_, then _P′_ is the point required.
If the lines, as in the figure, fall outside of your sheet of paper,
in order to draw them, it is necessary to attach other sheets of paper
to its edges. This is inconvenient, but must be done at first that
you may see your way clearly; and sometimes afterwards, though there
are expedients for doing without such extension in fast sketching.
It is evident, however, that no extension of surface could be of any
use to us, if the distance _TD_, instead of being 3½ feet, were 100
feet, or a mile, as it might easily be in a landscape.
It is necessary, therefore, to obtain some other means of
construction; to do which we must examine the principle of the
problem.
In the analysis of Fig. 2., in the introductory remarks, I used the
word “height” only of the tower, _QP_, because it was only to its
vertical height that the law deduced from the figure could be applied.
For suppose it had been a pyramid, as _OQP_, Fig. 52., then the image
of its side, _QP_, being, like every other magnitude, limited on the
glass _AB_ by the lines coming from its extremities, would appear only
of the length _Q′S_; and it is not true that _Q′S_ is to _QP_ as _TS_
is to _TP_. But if we let fall a vertical _QD_ from _Q_, so as to get
the vertical height of the pyramid, then it is true that _Q′S_ is to
_QD_ as _TS_ is to _TD_.
[Illustration: Fig. 52.]
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