Theory Points
section ‹ Points ›
text ‹This theory defines (1+3)-dimensional spacetime points. The first
coordinate is the time coordinate, and the remaining three coordinates
give the spatial component.›
theory Points
imports Sorts
begin
record 'a Point =
tval :: "'a"
xval :: "'a"
yval :: "'a"
zval :: "'a"
record 'a Space =
svalx :: "'a"
svaly :: "'a"
svalz :: "'a"
abbreviation tComponent :: "'a Point ⇒ 'a" where
"tComponent p ≡ tval p"
abbreviation sComponent :: "'a Point ⇒ 'a Space" where
"sComponent p ≡ ⦇ svalx = xval p, svaly = yval p, svalz = zval p ⦈"
abbreviation mkPoint :: "'a ⇒ 'a ⇒ 'a ⇒ 'a ⇒ 'a Point" where
"mkPoint t x y z ≡ ⦇ tval = t, xval = x, yval =y, zval = z ⦈"
abbreviation stPoint :: "'a ⇒ 'a Space ⇒ 'a Point" where
"stPoint t s ≡ mkPoint t (svalx s) (svaly s) (svalz s)"
abbreviation mkSpace :: "'a ⇒ 'a ⇒ 'a ⇒ 'a Space" where
"mkSpace x y z ≡ ⦇ svalx = x, svaly =y, svalz = z ⦈"
text ‹ Points have coordinates in the field of quantities,
and can be thought of as the end-points of
vectors pinned to the origin. We can translate and scale them,
define accumulation points, etc.›
class Points = Quantities
begin
abbreviation moveBy :: "'a Point ⇒ 'a Point ⇒ 'a Point" ("_ ⊕ _") where
"(p ⊕ q) ≡ ⦇ tval = tval p + tval q,
xval = xval p + xval q,
yval = yval p + yval q,
zval = zval p + zval q ⦈"
abbreviation movebackBy :: "'a Point ⇒ 'a Point ⇒ 'a Point" ("_ ⊖ _") where
"(p ⊖ q) ≡ ⦇ tval = tval p - tval q,
xval = xval p - xval q,
yval = yval p - yval q,
zval = zval p - zval q ⦈"
abbreviation sMoveBy :: "'a Space ⇒ 'a Space ⇒ 'a Space" ("_ ⊕s _") where
"(p ⊕s q) ≡ ⦇ svalx = svalx p + svalx q,
svaly = svaly p + svaly q,
svalz = svalz p + svalz q ⦈"
abbreviation sMovebackBy :: "'a Space ⇒ 'a Space ⇒ 'a Space" ("_ ⊖s _") where
"(p ⊖s q) ≡ ⦇ svalx = svalx p - svalx q,
svaly = svaly p - svaly q,
svalz = svalz p - svalz q ⦈"
abbreviation scaleBy :: "'a ⇒ 'a Point ⇒ 'a Point" ("_ ⊗ _") where
"scaleBy a p ≡ ⦇ tval = a*tval p, xval = a*xval p,
yval = a*yval p, zval = a*zval p⦈"
abbreviation sScaleBy :: "'a ⇒ 'a Space ⇒ 'a Space" (" _ ⊗s _") where
"sScaleBy a p ≡ ⦇ svalx = a*svalx p,
svaly = a*svaly p,
svalz = a*svalz p⦈"
abbreviation sOrigin :: "'a Space" where
"sOrigin ≡ ⦇ svalx = 0, svaly = 0, svalz = 0 ⦈"
abbreviation origin :: "'a Point" where
"origin ≡ ⦇ tval = 0, xval = 0, yval = 0, zval = 0 ⦈"
abbreviation tUnit :: "'a Point" where
"tUnit ≡ ⦇ tval = 1, xval = 0, yval = 0, zval = 0 ⦈"
abbreviation xUnit :: "'a Point" where
"xUnit ≡ ⦇ tval = 0, xval = 1, yval = 0, zval = 0 ⦈"
abbreviation yUnit :: "'a Point" where
"yUnit ≡ ⦇ tval = 0, xval = 0, yval = 1, zval = 0 ⦈"
abbreviation zUnit :: "'a Point" where
"zUnit ≡ ⦇ tval = 0, xval = 0, yval = 0, zval = 1 ⦈"
abbreviation timeAxis :: "'a Point set" where
"timeAxis ≡ { p . xval p = 0 ∧ yval p = 0 ∧ zval p = 0 }"
abbreviation onTimeAxis :: "'a Point ⇒ bool"
where "onTimeAxis p ≡ (p ∈ timeAxis)"
subsection ‹ Squared norms and separation functions ›
text ‹This theory defines squared norms and separations. We do not yet
define unsquared norms because we are not assuming here that quantities
necessarily have square roots.›
abbreviation norm2 :: "'a Point ⇒ 'a" where
"norm2 p ≡ sqr (tval p) + sqr (xval p) + sqr (yval p) + sqr (zval p)"
abbreviation sep2 :: "'a Point ⇒ 'a Point ⇒ 'a" where
"sep2 p q ≡ norm2 (p ⊖ q)"
abbreviation sNorm2 :: "'a Space ⇒ 'a" where
"sNorm2 s ≡ sqr (svalx s)
+ sqr (svaly s)
+ sqr (svalz s)"
abbreviation sSep2 :: "'a Point ⇒ 'a Point ⇒ 'a" where
"sSep2 p q ≡ sqr (xval p - xval q)
+ sqr (yval p - yval q)
+ sqr (zval p - zval q)"
abbreviation mNorm2 :: "'a Point ⇒ 'a" ("∥ _ ∥m")
where "∥ p ∥m ≡ sqr (tval p) - sNorm2 (sComponent p)"
subsection ‹ Topological concepts ›
text ‹We will need to define topological concepts like continuity and
affine approximation later, so here we define open balls and accumulation points.›
abbreviation inBall :: "'a Point ⇒ 'a ⇒ 'a Point ⇒ bool"
("_ within _ of _")
where "inBall q ε p ≡ sep2 q p < sqr ε"
abbreviation ball :: "'a Point ⇒ 'a ⇒ 'a Point set"
where "ball q ε ≡ { p . inBall q ε p }"
abbreviation accPoint :: "'a Point ⇒ 'a Point set ⇒ bool"
where "accPoint p s ≡ ∀ ε > 0. ∃ q ∈ s. (p ≠ q) ∧ (inBall q ε p)"
subsection ‹ Lines ›
text ‹ A line is specified by giving a point on the line,
and a point (thought of as a vector) giving its direction. For
these purposes it doesn't matter whether the direction is "positive"
or "negative". ›
abbreviation line :: "'a Point ⇒ 'a Point ⇒ 'a Point set"
where "line base drtn ≡ { p . ∃ α . p = (base ⊕ (α⊗drtn)) }"
abbreviation lineJoining :: "'a Point ⇒ 'a Point ⇒ 'a Point set"
where "lineJoining p q ≡ line p (q⊖p)"
abbreviation isLine :: "'a Point set ⇒ bool"
where "isLine l ≡ ∃ b d . (l = line b d)"
abbreviation sameLine :: "'a Point set ⇒ 'a Point set ⇒ bool"
where "sameLine l1 l2 ≡ ((isLine l1) ∨ (isLine l2)) ∧ (l1 = l2)"
abbreviation onLine :: "'a Point ⇒ 'a Point set ⇒ bool"
where "onLine p l ≡ (isLine l) ∧ (p ∈ l)"
subsection ‹ Directions ›
text ‹ Given any two distinct points on a line, the vector joining them
can be used to specify the line's direction. The direction of a line is
therefore a \emph{set} of points/vectors. By lemDrtn these are all parallel ›
fun drtn :: "'a Point set ⇒ 'a Point set"
where "drtn l = { d . ∃ p q . (p ≠ q) ∧ (onLine p l) ∧ (onLine q l) ∧ (d = (q ⊖ p)) }"
abbreviation parallelLines :: "'a Point set ⇒ 'a Point set ⇒ bool"
where "parallelLines l1 l2 ≡ (drtn l1) ∩ (drtn l2) ≠ {}"
abbreviation parallel :: "'a Point ⇒ 'a Point ⇒ bool" (" _ ∥ _ ")
where "parallel p q ≡ (∃ α ≠ 0 . p = (α ⊗ q))"
text ‹The "slope" of a line can be either finite or infinite. We will often
need to consider these two cases separately.›
abbreviation slopeFinite :: "'a Point ⇒ 'a Point ⇒ bool"
where "slopeFinite p q ≡ (tval p ≠ tval q)"
abbreviation slopeInfinite :: "'a Point ⇒ 'a Point ⇒ bool"
where "slopeInfinite p q ≡ (tval p = tval q)"
abbreviation lineSlopeFinite :: "'a Point set ⇒ bool"
where "lineSlopeFinite l ≡ (∃ x y . (onLine x l) ∧ (onLine y l)
∧ (x ≠ y) ∧ (slopeFinite x y))"
subsection ‹ Slopes and slopers ›
text ‹We specify the slope of a line by giving the spatial component ("sloper")
of the point on the line at time 1. This is defined if and only if the slope is finite.
If the slope is infinite (the line is "horizontal") we return the spatial origin. This
avoids using "option" but means we need to consider carefully whether a sloper with
value sOrigin indicates a truly zero slope or an infinite one.›
fun sloper :: "'a Point ⇒ 'a Point ⇒ 'a Point"
where "sloper p q = (if (slopeFinite p q) then ((1 / (tval p - tval q)) ⊗ (p ⊖ q))
else origin)"
fun velocityJoining :: "'a Point ⇒ 'a Point ⇒ 'a Space"
where "velocityJoining p q = sComponent (sloper p q)"
fun lineVelocity :: "'a Point set ⇒ 'a Space set"
where "lineVelocity l = { v . ∃ d ∈ drtn l . v = velocityJoining origin d }"
lemma lemNorm2Decomposition:
shows "norm2 u = sqr (tval u) + sNorm2 (sComponent u)"
by (simp add: add_commute local.add.left_commute)
lemma lemPointDecomposition:
shows "p = (((tval p)⊗tUnit) ⊕ (((xval p)⊗xUnit)
⊕ (((yval p)⊗yUnit) ⊕ ((zval p)⊗zUnit))))"
by force
lemma lemScaleLeftSumDistrib: "((a + b) ⊗ p) = ((a⊗p) ⊕ (b⊗p))"
using distrib_right by auto
lemma lemScaleLeftDiffDistrib: "((a - b) ⊗ p) = ((a⊗p) ⊖ (b⊗p))"
using left_diff_distrib by auto
lemma lemScaleAssoc: "(α ⊗ (β ⊗ p)) = ((α * β) ⊗ p)"
using semiring_normalization_rules(18) by auto
lemma lemScaleCommute: "(α ⊗ (β ⊗ p)) = (β ⊗ (α ⊗ p))"
using mult.left_commute by auto
lemma lemScaleDistribSum: "(α ⊗ (p ⊕ q)) = ((α⊗p) ⊕ (α⊗q))"
using distrib_left by auto
lemma lemScaleDistribDiff: "(α ⊗ (p ⊖ q)) = ((α⊗p) ⊖ (α⊗q))"
using right_diff_distrib by auto
lemma lemScaleOrigin: "(α ⊗ origin) = origin"
by auto
lemma lemMNorm2OfScaled: "mNorm2 (scaleBy α p) = (sqr α) * mNorm2 p"
using lemSqrMult distrib_left right_diff_distrib' by simp
lemma lemSNorm2OfScaled: "sNorm2 (sScaleBy α p) = (sqr α) * sNorm2 p"
using lemSqrMult distrib_left by auto
lemma lemNorm2OfScaled: "norm2 (α ⊗ p) = (sqr α) * norm2 p"
using lemSqrMult distrib_left by auto
lemma lemScaleSep2: "(sqr a) * (sep2 p q) = sep2 (a⊗p) (a⊗q)"
using lemNorm2OfScaled[of "a" "p⊖q"] lemScaleDistribDiff by auto
lemma lemSScaleAssoc: "(α ⊗s (β ⊗s p)) = ((α * β) ⊗s p)"
using semiring_normalization_rules(18) by auto
lemma lemScaleBall:
assumes "x within e of y"
and "a ≠ 0"
shows "(a⊗x) within (a*e) of (a⊗y)"
proof -
have a2pos: "sqr a > 0" using assms(2) lemSquaresPositive by auto
have "sep2 (a⊗x) (a⊗y) = (sqr a) * (sep2 x y)" using lemScaleSep2 by auto
hence "sep2 (a⊗x) (a⊗y) < (sqr a) * (sqr e)"
using assms mult_strict_left_mono a2pos by auto
thus ?thesis using mult_commute mult_assoc by auto
qed
lemma lemScaleBallAndBoundary:
assumes "sep2 x y ≤ sqr e"
and "a ≠ 0"
shows "sep2 (a⊗x) (a⊗y) ≤ sqr (a*e)"
proof -
have a2pos: "sqr a > 0" using assms(2) lemSquaresPositive by auto
have "sep2 (a⊗x) (a⊗y) = (sqr a) * (sep2 x y)" using lemScaleSep2 by auto
hence "sep2 (a⊗x) (a⊗y) ≤ (sqr a) * (sqr e)"
using assms mult_left_mono a2pos by auto
thus ?thesis using mult_commute mult_assoc by auto
qed
lemma lemTimeAxisIsLine: "isLine timeAxis"
proof -
{ fix p
{ assume p: "p ∈ timeAxis"
hence "p = (origin ⊕ ((tval p) ⊗ tUnit))" by auto
}
hence l2r: "onTimeAxis p ⟶ (∃ v . (p = (origin ⊕ (v ⊗ tUnit))))" by blast
{ assume v: "∃ v . p = (origin ⊕ (v ⊗ tUnit))"
hence "onTimeAxis p" by auto
}
hence "(∃ v . (p = (origin ⊕ (v ⊗ tUnit)))) ⟷ onTimeAxis p"
using l2r by blast
}
hence "timeAxis = line origin tUnit" by blast
thus ?thesis by blast
qed
lemma lemSameLine:
assumes "p ∈ line b d"
shows "sameLine (line b d) (line p d)"
proof -
define l1 where l1: "l1 = line b d"
define l2 where l2: "l2 = line p d"
have lines: "isLine l1 ∧ isLine l2" using l1 l2 by blast
obtain A where p: "p = (b ⊕ (A ⊗ d))" using assms by auto
hence b: "b = (p ⊖ (A ⊗ d))" by auto
{ fix x
{ assume x: "x ∈ l1"
then obtain a where a: "x = (b ⊕ (a⊗d))" using l1 by auto
hence "x = ((p ⊖ (A ⊗ d)) ⊕ (a⊗d))" using b by simp
also have "… = (p ⊕ ((a⊗d)⊖(A⊗d)))"
using add_diff_eq diff_add_eq add_commute add_assoc by simp
finally have "x = (p ⊕ ((a-A)⊗d))"
using lemScaleLeftDiffDistrib by presburger
hence "x ∈ l2" using l2 by auto
}
hence l2r: "(x ∈ l1) ⟶ (x ∈ l2)" using l2 by simp
{ assume x: "x ∈ l2"
then obtain a where a: "x = (p ⊕ (a ⊗ d))" using l2 by auto
hence "x = (b ⊕ ((A+ a)⊗d))"
using p add_assoc lemScaleAssoc distrib by auto
hence "x ∈ l1" using l1 by auto
}
hence "(x ∈ l1) ⟷ (x ∈ l2)" using l2r by auto
}
thus ?thesis using lines l1 l2 by auto
qed
lemma lemSSep2Symmetry: "sSep2 p q = sSep2 q p"
using lemSqrDiffSymmetrical by simp
lemma lemSep2Symmetry: "sep2 p q = sep2 q p"
using lemSqrDiffSymmetrical by simp
lemma lemSpatialNullImpliesSpatialOrigin:
assumes "sNorm2 s = 0"
shows "s = sOrigin"
using assms local.add_nonneg_eq_0_iff by auto
lemma lemNorm2NonNeg: "norm2 p ≥ 0"
by simp
lemma lemNullImpliesOrigin:
assumes "norm2 p = 0"
shows "p = origin"
proof -
have "norm2 p = sqr (tval p) + sNorm2 (sComponent p)" using add_assoc by simp
hence a: "sqr (tval p) + sNorm2 (sComponent p) = 0" using assms by auto
{ assume b: "sNorm2 (sComponent p) > 0"
have "sqr (tval p) + sNorm2 (sComponent p) > 0"
using b lemSumOfNonNegAndPos by auto
hence "False" using a by auto
}
hence c: "¬(sNorm2 (sComponent p) > 0)" by auto
have d: "sNorm2 (sComponent p) ≥ 0" by auto
have "∀ x . (¬(x > 0)) ∧ (x ≥ 0) ⟶ x = 0" by auto
hence e: "sNorm2 (sComponent p) = 0" using c d by force
hence f: "sComponent p = sOrigin"
using lemSpatialNullImpliesSpatialOrigin by blast
have "norm2 p = sqr (tval p)" using e add_assoc by auto
hence "sqr (tval p) = 0" using assms by simp
hence "(tval p) = 0" using lemZeroRoot by simp
thus ?thesis using f by auto
qed
lemma lemNotOriginImpliesPosNorm2:
assumes "p ≠ origin"
shows "norm2 p > 0"
proof -
have 1: "norm2 p ≥ 0" by simp
have 2: "norm2 p ≠ 0" using assms(1) lemNullImpliesOrigin by force
thus ?thesis using 1 2 dual_order.not_eq_order_implies_strict by fast
qed
lemma lemNotEqualImpliesSep2Pos:
assumes "y ≠ x"
shows "sep2 y x > 0"
proof -
have "(y⊖x) ≠ origin" using assms by auto
hence 1: "norm2 (y⊖x) > 0" using lemNotOriginImpliesPosNorm2 by fast
have "sep2 y x = norm2 (y⊖x)" by auto
thus ?thesis using 1 by auto
qed
lemma lemBallContainsCentre:
assumes "ε > 0"
shows "x within ε of x"
proof -
have "sep2 x x = 0" by auto
thus ?thesis using assms by auto
qed
lemma lemPointLimit:
assumes "∀ ε > 0 . (v within ε of u)"
shows "v = u"
proof -
define d where d: "d = sep2 v u"
{ assume "v ≠ u"
hence "d > 0" using lemNotEqualImpliesSep2Pos d by auto
then obtain s where s: "(0 < s) ∧ (sqr s < d)" using lemSmallSquares by auto
hence "v within s of u" using d assms(1) by auto
hence "sep2 v u < sep2 v u" using s d by auto
hence "False" by auto
}
thus ?thesis by auto
qed
lemma lemBallPopulated:
assumes "e > 0"
shows "∃ y . (y within e of x) ∧ (y ≠ x)"
proof -
obtain e1 where e1: "(0 < e1) ∧ (e1 < e) ∧ (sqr e1 < e1)"
using assms lemReducedBound by auto
hence e2: "sqr e1 < sqr e" using lemSqrMonoStrict[of "e1" "e"] by auto
define y where y: "y = (x ⊕ ⦇ tval = e1, xval=0, yval=0, zval=0 ⦈)"
hence "(y ⊖ x) = ⦇ tval = e1, xval=0, yval=0, zval=0 ⦈" by auto
hence "sep2 y x = sqr e1" by auto
hence 1: "y within e of x" using e2 by auto
have "tval y = tval x + e1" using y by simp
hence "y ≠ x" using e1 by auto
thus ?thesis using 1 by auto
qed
lemma lemBallInBall:
assumes "p within x of q"
and "0 < x ≤ y"
shows "p within y of q"
proof -
have "sqr x ≤ sqr y" using assms(2) lemSqrMono by auto
thus ?thesis using le_less_trans using assms(1) by auto
qed
lemma lemSmallPoints:
assumes "e > 0"
shows "∃ a > 0 . norm2 (a⊗p) < sqr e"
proof -
{ assume po: "p = origin"
define a where a: "a = 1"
hence apos: "a > 0" by auto
have "norm2 (a⊗p) < sqr e" using a po assms by auto
hence ?thesis using apos by auto
}
hence case1: "p = origin ⟶ ?thesis" by auto
{ assume pnoto: "p ≠ origin"
obtain e1 where e1: "(e1 > 0) ∧ (e1 < e) ∧ (sqr e1 < e1)"
using lemReducedBound assms by auto
hence e1sqr: "0 < (sqr e1) < (sqr e)" using lemSqrMonoStrict by auto
define n2 where n2: "n2 = norm2 p"
hence n2pos: "n2 > 0" using pnoto lemNotOriginImpliesPosNorm2 by auto
then obtain s where s: "(s > 0) ∧ (sqr s > n2)"
using lemSquareExistsAbove by auto
hence "0 < (n2/(sqr s)) < 1" using n2pos by auto
hence "(sqr e1)*(n2/(sqr s)) < sqr e1"
using lemMultPosLT1[of "sqr e1" "(n2/(sqr s))"] e1sqr by auto
hence ineq: "(sqr e1)*(n2/(sqr s)) < sqr e" using e1sqr by auto
define a where a: "a = e1/s"
have "e1 > 0 ∧ s > 0" using e1 s by auto
hence apos: "a > 0" using a by auto
have "norm2 (a⊗p) = (sqr e1)*(n2/(sqr s))"
using lemNorm2OfScaled[of "a"] a n2 by auto
hence "norm2 (a⊗p) < sqr e" using ineq by auto
hence ?thesis using apos by auto
}
hence "p ≠ origin ⟶ ?thesis" by auto
thus ?thesis using case1 by auto
qed
lemma lemLineJoiningContainsEndPoints:
assumes "l = lineJoining x p"
shows "onLine x l ∧ onLine p l"
proof -
have line: "isLine l" using assms(1) by blast
have p: "x = (x ⊕ (0 ⊗ (p⊖x)))" by simp
have x: "p = (x ⊕ (1 ⊗ (p⊖x)))" using add_commute diff_add_cancel by fastforce
thus ?thesis using p line assms(1) by blast
qed
lemma lemLineAndPoints:
assumes "p ≠ q"
shows "(onLine p l ∧ onLine q l) ⟷ (l = lineJoining p q)"
proof -
define lj where lj : "lj = lineJoining p q"
define lhs where lhs: "lhs = (onLine p l ∧ onLine q l)"
define rhs where rhs: "rhs = (l = lj)"
{ assume hyp: "lhs"
then obtain b d where bd: "l = { x. ∃ a. x = (b ⊕ (a⊗d)) }" using lhs by auto
obtain ap where ap: "p = (b ⊕ (ap ⊗ d))" using hyp lhs bd by auto
obtain aq where aq: "q = (b ⊕ (aq ⊗ d))" using hyp lhs bd by auto
hence "(q⊖p) = ((b ⊕ (aq ⊗ d)) ⊖ (b ⊕ (ap ⊗ d)))" using ap by fast
also have "... = ((aq ⊗ d) ⊖ (ap ⊗ d))" using add_diff_cancel by auto
finally have qdiffp: "(q⊖p) = ((aq - ap) ⊗ d)"
using lemScaleLeftDiffDistrib[of "aq" "ap" "d"] by auto
define R where R: "R = aq - ap"
hence Rnz: "R ≠ 0" using assms(1) qdiffp by auto
define r where r: "r = 1/R"
hence "(r⊗(R ⊗ d)) = (r ⊗ (q⊖p))" using R qdiffp by auto
hence d: "d = (r ⊗ (q⊖p))" using lemScaleAssoc[of "r" "R" "d"] r Rnz by force
have "b = (p ⊖ (ap ⊗ d))" using ap by auto
also have "... = (p ⊖ (ap ⊗ (r ⊗ (q⊖p))))" using d by auto
finally have b: "b = (p ⊖ ( (ap*r) ⊗ (q⊖p)))"
using lemScaleAssoc[of "ap" "r" "q⊖p"] by auto
{ fix x
assume "x ∈ l"
then obtain a where "x = (b ⊕ (a ⊗ d))" using bd by auto
hence "x = ((p ⊖ ((ap*r) ⊗ (q⊖p))) ⊕ ((a*r) ⊗ (q⊖p)))"
using b d lemScaleAssoc[of "a" "r" "q⊖p"] by fastforce
also have "... = (p ⊕ ( ((a*r)⊗(q⊖p)) ⊖ ((ap*r)⊗(q⊖p)) ))"
using add_diff_eq diff_add_eq by force
also have "... = (p ⊕ (((a*r)-(ap*r))⊗(q⊖p)))"
using left_diff_distrib by force
finally have "x ∈ lj" using lj by auto
}
hence l2r: "l ⊆ lj" by auto
{ fix x
assume "x ∈ lj"
then obtain a where a: "x = (p ⊕ (a ⊗(q⊖p)))" using lj by auto
hence "x = ((b ⊕ (ap ⊗ d)) ⊕ (a ⊗(R ⊗ d)))" using ap qdiffp R by auto
also have "... = (b ⊕ ((ap + a*R)⊗d))"
using add_assoc distrib_right lemScaleAssoc
by auto
finally have "onLine x l" using bd by auto
}
hence "lj ⊆ l" by auto
hence "l = lj" using l2r by auto
}
hence L2R: "lhs ⟶ rhs" using rhs by auto
{ assume l: "rhs"
hence line: "isLine l" using rhs lj by blast
have p: "p = (p ⊕ (0 ⊗ (q⊖p)))" by simp
have q: "q = (p ⊕ (1 ⊗ (q⊖p)))" using add_commute diff_add_cancel by fastforce
hence "lhs" using p line l lhs rhs lj by blast
}
hence "rhs ⟶ lhs" by auto
hence "lhs ⟷ rhs" using L2R by auto
thus ?thesis using lhs rhs lj by auto
qed
lemma lemLineDefinedByPair:
assumes "x ≠ p"
and "(onLine p l1) ∧ (onLine x l1)"
and "(onLine p l2) ∧ (onLine x l2)"
shows "l1 = l2"
proof -
have "l1 = lineJoining x p"
using lemLineAndPoints[of "x" "p" "l1"] assms(1) assms(2) by auto
also have "... = l2"
using lemLineAndPoints[of "x" "p" "l2"] assms(1) assms(3) by auto
finally show "l1 = l2" by auto
qed
lemma lemDrtn:
assumes "{ d1, d2 } ⊆ drtn l"
shows "∃ α ≠ 0 . d2 = (α ⊗ d1)"
proof -
have d1d2: "{d1,d2} ⊆ { d . ∃ p q . (p ≠ q) ∧ onLine p l ∧ onLine q l ∧ (d = (q ⊖ p)) }"
using assms(1) by auto
have d1: "∃ p1 q1 . (p1 ≠ q1) ∧ (onLine p1 l) ∧ (onLine q1 l) ∧ (d1 = (q1 ⊖ p1))"
using d1d2 by auto
then obtain p1 q1
where pq1: "(p1 ≠ q1) ∧ (onLine p1 l) ∧ (onLine q1 l) ∧ (d1 = (q1 ⊖ p1))"
by blast
hence l1: "l = lineJoining p1 q1" using lemLineAndPoints[of "p1" "q1" "l"] by auto
have d2: "∃ p2 q2 . (p2 ≠ q2) ∧ (onLine p2 l) ∧ (onLine q2 l) ∧ (d2 = (q2 ⊖ p2))"
using d1d2 by auto
then obtain p2 q2
where pq2: "(p2 ≠ q2) ∧ (onLine p2 l) ∧ (onLine q2 l) ∧ (d2 = (q2 ⊖ p2))"
by blast
hence "(p2 ∈ lineJoining p1 q1) ∧ (q2 ∈ lineJoining p1 q1)" using l1 by blast
then obtain ap aq
where apaq: "(p2 = (p1 ⊕ (ap⊗(q1⊖p1)))) ∧ ((q2 = (p1 ⊕ (aq⊗(q1⊖p1)))))"
by blast
define diff where diff: "diff = aq - ap"
hence diffnz: "diff ≠ 0" using apaq pq2 by auto
have "d2 = (q2 ⊖ p2)" using pq2 by simp
also have "... = ((p1 ⊕ (aq⊗(q1⊖p1))) ⊖ (p1 ⊕ (ap⊗(q1⊖p1))))" using apaq by force
also have "... = ((aq⊗(q1⊖p1)) ⊖ (ap⊗(q1⊖p1)))" by auto
also have "... = ((aq - ap) ⊗ d1)"
using pq1 lemScaleLeftDiffDistrib[ of "aq" "ap" "d1"] by auto
finally have "(d2 = (diff ⊗ d1)) ∧ (diff ≠ 0)" using diff diffnz by auto
thus ?thesis by auto
qed
lemma lemLineDeterminedByPointAndDrtn:
assumes "(x ≠ p) ∧ (p ∈ l1) ∧ (onLine x l1) ∧ (onLine x l2)"
and "drtn l1 = drtn l2"
shows "l1 = l2"
proof -
define d1 where d1: "d1 = drtn l1"
define d2 where d2: "d2 = drtn l2"
hence dd: "d1 = d2" using assms(2) d1 by auto
define px where px: "px = (p ⊖ x)"
have l1: "(x ≠ p) ∧ (onLine p l1) ∧ (onLine x l1)" using assms(1) by auto
hence "∃ p q . (p ≠ q) ∧ onLine p l1 ∧ onLine q l1 ∧ (px = (q ⊖ p))" using px by blast
hence "px ∈ { d . ∃ p q . (p ≠ q) ∧ onLine p l1 ∧ onLine q l1 ∧ (d = (q ⊖ p)) }"
by blast
hence "px ∈ d1" using d1 subst[of "d1" "drtn l1" "λs. px ∈ s"] by auto
hence "px ∈ d2" using dd by simp
hence pxonl2: "px ∈ drtn l2" using d2 by simp
hence "∃ u v . (u ≠ v) ∧ onLine u l2 ∧ onLine v l2 ∧ (px = (v ⊖ u))" by auto
then obtain u v where uv: "(u ≠ v) ∧ onLine u l2 ∧ onLine v l2 ∧ (px = (v ⊖ u))" by blast
hence "(x ≠ u) ∨ (x ≠ v)" by blast
then obtain w where w: "((w = u) ∨ (w = v)) ∧ (x ≠ w)" by blast
hence xw: "(x ≠ w) ∧ (onLine x l2) ∧ (onLine w l2)" using uv assms(1) by blast
hence l2: "l2 = lineJoining x w" using lemLineAndPoints[of "x" "w" "l2"] by auto
hence "(w ⊖ x) ∈ drtn l2 ∧ px ∈ drtn l2" using xw pxonl2 by auto
then obtain a where a: "(a ≠ 0) ∧ (p ⊖ x) = (a ⊗ (w ⊖ x))"
using lemDrtn[of "w⊖x" "p⊖x" "l2"] px xw pxonl2 by blast
hence "p = (x ⊕ (a ⊗ (w ⊖ x)))" by (auto simp add: field_simps)
hence "onLine p (lineJoining x w)" by blast
hence l2lj: "l2 = lineJoining x p"
using lemLineAndPoints[of "x" "p" "l2"] assms(1) l2 xw
by auto
have l1lj: "l1 = lineJoining x p"
using lemLineAndPoints[of "x" "p" "l1"] assms(1)
by auto
thus ?thesis using l2lj by blast
qed
end
end