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chapter 1 | The Necessity of Perspective
chapter 1 | The Necessity of Perspective
chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle
In a given plane, the perceived length of an object depends on the pair of light rays emanating from the two points of the object in that plane that subtend the greatest angle at the eye.  chapter 2 | Collinearity and Angle
chapter 2 | Collinearity and Angle Points that are collinear with the eye will appear to share the same position, and hence, appear to be the same point.
The apparent dimension of an object does not depend directly on what its actual dimension is, nor at what distance from the eye it is placed. It depends directly on one, and only one thing: the angle subtended by it at the eye. The larger this angle compared to the angles of other objects, the larger it will look compared to them. chapter 2 | Collinearity and Angle
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3 | The Linear and Planar Scales
chapter 3.1 | Size
chapter 3.1 | Size
	There’s a car whose breadth is 2 meters, and you hold a scale about 10 cm from your eye.  	100 m away, 	1 m away, 10,000 times! chapter 3.1 | Size
chapter 3.1 | Size l’∝ df
chapter 3.1 | Size
chapter 3.1 | Size 5.1 mm, 1 m away
chapter 3.1 | Size n∆l,  n∆l’
chapter 3.1 | Size
chapter 3.1 | Size
chapter 3.2 | Position
chapter 3.2 | Position In ΔOP’N’, tanθ = x’/df⇒x’ =dftanθ.
chapter 3.2 | Position
chapter 3.2 | Position
chapter 3.2 | Position θ’ = θ.
? chapter 3.2 | Position (r’, θ’)  ≡ But the vanishing point is not always  at the centre, along our line of sight.
chapter 3.2 | Position Use this with functions f(x,y,z,t) to project objects at a single go. E = E(t)
chapter 3.2 | Position
chapter 3.2 | Position
chapter 3.3 | Motion For non-planar displacements, project end-points, then join.
chapter 3.3 | Motion
chapter 3.3 | Motion
chapter 3.3 | Motion
Review of Part 1
Review of Part 1
chapter 3.4.1 | Applications: The Cube A cube of side-length 50cm dx = 20cm dy = 30cm dz = 1m The reference frame is at a distance df  = 10cm, and graduated in meters.
chapter 3.4.1 | Applications: The Cube
chapter 3.4.1 | Applications: The Cube
? chapter 3.4.1 | Applications: The Cube But is it correct to just join the projected corners?
chapter 3.4.1 | Applications: The Straight Line x’ {m (ez- z1) – n (ey- y1)} – df m (ex - x1) = y’ {l (ez- z1) – n (ex - x1)} - df l (ey- y1).
chapter 3.4.1 | Applications: The Straight Line ,
chapter 3.4.1 | Applications: The Straight Line (x’, y’) ≡  (x’, y’, df) = (x’ n/df, y’ n/df, n) = (l, m, n)
chapter 3.4.1 | Applications: The Straight Line
chapter 3.4.1 | Applications: The Straight Line l1l2+m1m2+n1n2 = l1l3+m1m3+n1n3 = l2l3+m2m3+n2n3 = 0. x1x2 + y1y2 = x1x3 + y1y3 = x2x3 + y2y3 = -df2.
chapter 3.4.1 | Applications: The Straight Line v1 (x1, y1) v2 (x2, y2) v3 (x3, y3) v1.v2 = v1.v3 ⇒ v1.(v2-v3) = 0.
chapter 3.4.1 | Applications: The Straight Line v1 v2 v3
chapter 3.4.2 | Applications: The Wall z = mx + d, y = ±h.
chapter 3.4.2 | Applications: The Wall d = 2m h = 1.5m df = 10cm θ = 60°
chapter 3.4.3 | Applications: The Staircase 20 steps
chapter 3.4.3 | Applications: The Staircase 10 steps above eye level 7 steps below
chapter 3.4.3 | Applications: The Staircase Till the 9th step below
chapter 3.4.3 | Applications: The Staircase The 10th step
chapter 3.4.3 | Applications: The Staircase
chapter 3.4.4 | Applications: The Circle r = R, z= do
chapter 3.4.4 | Applications: The Circle x2 + y2 + (z-d)2 = r2, z = mx + d
chapter 3.4.4 | Applications: The Circle
chapter 3.4.4 | Applications: The Circle
chapter 3.4.5 | Applications: The Sphere x2 + y2 + (z-d)2 = r2 The perceived size of an object depends on the pairs of light rays emanating from it that subtend the greatest angle at the eye.
chapter 3.4.5 | Applications: The Sphere
chapter 3.4.5 | Applications: The Sphere
P’: (x’, y’) chapter 3.5 | Working Backwards: From Image to Object
chapter 3.5 | Working Backwards: From Image to Object r’ = R
chapter 3.4.5 | Binocular Vision
? chapter 3.4.5 | Binocular Vision (x, y, z) ≡  But does your brain know this formula?
chapter 3.4.5 | Binocular Vision
chapter 4 | The Circular and Spherical Scales
chapter 4 | The Circular and Spherical Scales
chapter 4.1 | Position x’ =rfθ
chapter 4.1 | Position
chapter 4.2 | Applications: The Wall z = d, y = ±h But this graph is WRONG!
chapter 4.2 | Applications: The Wall
chapter 4.2 | Applications: The Wall
chapter 5 | The Cylindrical Scale
chapter 5.1 | Position
chapter 5.2 | Applications: The Wall z = d, y = ±h
chapter 5.2 | Applications: The Wall
chapter 6| The Semicircular and Hemispherical Scales
chapter 6.1 | Position
chapter 6.2 | Applications: The Wall z = d, y = ±h
chapter 6.2 | Applications: The Wall
chapter 7| More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
chapter 7 | More on Binocular Vision
Microsoft© Word TM and PowerPoint TM MathCast Copyright © 2004-2007 Tom Chakam    www.mathcast.sf.net MathGV Graph   www.padowan.dk MetaCreations Bryce 4 Adobe© Photoshop TM Credits

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Perspective: the maths of seeing