Linear-Algebra-Done-Right Β· Unit 17 Β· Video 1 Β· Interactive Practice
The Closest Point Is the Projection: Fitting Sine on [βΟ, Ο]
I Key Formulas
Key Insight: Projecting sin β‘ \sin sin onto P 5 ( R ) \mathcal{P}_5(\mathbf{R}) P 5 β ( R ) gives u ( x ) = 0.987862 x β 0.155271 x 3 + 0.00564312 x 5 u(x) = 0.987862x - 0.155271x^3 + 0.00564312x^5 u ( x ) = 0.987862 x β 0.155271 x 3 + 0.00564312 x 5 , the degree-5 polynomial with the smallest β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x \int_{-\pi}^{\pi} |\sin x - u(x)|^2\,dx β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x β the theorem guarantees the integral, not the error at each point.
II The Closest Point Is the Foot of the Perpendicular
For every u β U u \in U u β U , the legs v β P U v v - P_U v v β P U β v and P U v β u P_U v - u P U β v β u are orthogonal, so β₯ v β u β₯ \|v - u\| β₯ v β u β₯ is a hypotenuse.
III Projecting sin β‘ \sin sin onto P 5 ( R ) \mathcal{P}_5(\mathbf{R}) P 5 β ( R ) One Term at a Time
Each orthonormal term β¨ sin β‘ , e k β© e k \langle \sin, e_k \rangle e_k β¨ sin , e k β β© e k β lowers the squared error by exactly β¨ sin β‘ , e k β© 2 \langle \sin, e_k \rangle^2 β¨ sin , e k β β© 2 .
βΆ play
Terms k 0
e 1 = 0.398942 e_1 = 0.398942 e 1 β = 0.398942 is even, so β¨ sin β‘ , e 1 β© = 0 \langle \sin, e_1 \rangle = 0 β¨ sin , e 1 β β© = 0 .
e 2 = 0.219948 x e_2 = 0.219948x e 2 β = 0.219948 x is odd, and β¨ sin β‘ , e 2 β© = 1.38198 \langle \sin, e_2 \rangle = 1.38198 β¨ sin , e 2 β β© = 1.38198 .
e 3 = 0.135577 x 2 β 0.446031 e_3 = 0.135577x^2 - 0.446031 e 3 β = 0.135577 x 2 β 0.446031 is even, so β¨ sin β‘ , e 3 β© = 0 \langle \sin, e_3 \rangle = 0 β¨ sin , e 3 β β© = 0 .
e 4 = 0.0851039 x 3 β 0.503965 x e_4 = 0.0851039x^3 - 0.503965x e 4 β = 0.0851039 x 3 β 0.503965 x is odd, and β¨ sin β‘ , e 4 β© = β 1.09734 \langle \sin, e_4 \rangle = -1.09734 β¨ sin , e 4 β β© = β 1.09734 .
e 5 = 0.0537539 x 4 β 0.454740 x 2 + 0.448810 e_5 = 0.0537539x^4 - 0.454740x^2 + 0.448810 e 5 β = 0.0537539 x 4 β 0.454740 x 2 + 0.448810 is even, so β¨ sin β‘ , e 5 β© = 0 \langle \sin, e_5 \rangle = 0 β¨ sin , e 5 β β© = 0 .
e 6 = 0.0340493 x 5 β 0.373392 x 3 + 0.789692 x e_6 = 0.0340493x^5 - 0.373392x^3 + 0.789692x e 6 β = 0.0340493 x 5 β 0.373392 x 3 + 0.789692 x is odd, and β¨ sin β‘ , e 6 β© = 0.165734 \langle \sin, e_6 \rangle = 0.165734 β¨ sin , e 6 β β© = 0.165734 .
IV Projection Versus Taylor
The projection minimizes the integrated squared error, yet the Taylor polynomial still wins pointwise near x = 0 x = 0 x = 0 .
Degree
1
3
5
Probe x 3.00
V Quiz Questions
Problem 1 Β· Distance to a Plane
Given: In R 3 \mathbf{R}^3 R 3 with the dot product, U = span β‘ ( e 1 , e 2 ) U = \operatorname{span}(e_1, e_2) U = span ( e 1 β , e 2 β ) where e 1 = 1 2 ( 1 , 1 , 0 ) e_1 = \tfrac{1}{\sqrt{2}}(1, 1, 0) e 1 β = 2 β 1 β ( 1 , 1 , 0 ) and e 2 = ( 0 , 0 , 1 ) e_2 = (0, 0, 1) e 2 β = ( 0 , 0 , 1 ) are orthonormal, and v = ( 3 , 1 , 2 ) v = (3, 1, 2) v = ( 3 , 1 , 2 ) . Find min β‘ u β U β₯ v β u β₯ \min_{u \in U} \|v - u\| min u β U β β₯ v β u β₯ .
a 2 2 2
b 14 \sqrt{14} 14 β
c 2 \sqrt{2} 2 β
d 2 3 2\sqrt{3} 2 3 β
β
Correct! P U v = ( 2 , 2 , 2 ) P_U v = (2, 2, 2) P U β v = ( 2 , 2 , 2 ) , so the minimum is
β₯ v β P U v β₯ = β₯ ( 1 , β 1 , 0 ) β₯ = 2 \|v - P_U v\| = \|(1, -1, 0)\| = \sqrt{2} β₯ v β P U β v β₯ = β₯ ( 1 , β 1 , 0 ) β₯ = 2 β .
β Not quite. 2 2 2 is the squared distance
β₯ v β P U v β₯ 2 \|v - P_U v\|^2 β₯ v β P U β v β₯ 2 ; take its square root.
β Not quite. 14 = β₯ v β₯ = β₯ v β 0 β₯ \sqrt{14} = \|v\| = \|v - 0\| 14 β = β₯ v β₯ = β₯ v β 0β₯ is the distance to one particular point of
U U U , the origin, not the closest one.
β Not quite. 2 3 = β₯ P U v β₯ 2\sqrt{3} = \|P_U v\| 2 3 β = β₯ P U β v β₯ is the length of the projection itself; the distance is the length of the perpendicular piece
v β P U v v - P_U v v β P U β v .
Show solution
By the theorem the closest point is P U v P_U v P U β v , computed with the orthonormal basis:
β¨ v , e 1 β© = 3 + 1 2 = 2 2 , β¨ v , e 2 β© = 2 , \langle v, e_1 \rangle = \tfrac{3 + 1}{\sqrt{2}} = 2\sqrt{2}, \qquad \langle v, e_2 \rangle = 2, β¨ v , e 1 β β© = 2 β 3 + 1 β = 2 2 β , β¨ v , e 2 β β© = 2 ,
P U v = 2 2 β
1 2 ( 1 , 1 , 0 ) + 2 ( 0 , 0 , 1 ) = ( 2 , 2 , 2 ) . P_U v = 2\sqrt{2}\cdot\tfrac{1}{\sqrt{2}}(1, 1, 0) + 2(0, 0, 1) = (2, 2, 2). P U β v = 2 2 β β
2 β 1 β ( 1 , 1 , 0 ) + 2 ( 0 , 0 , 1 ) = ( 2 , 2 , 2 ) .
Then v β P U v = ( 1 , β 1 , 0 ) v - P_U v = (1, -1, 0) v β P U β v = ( 1 , β 1 , 0 ) , which is orthogonal to both e 1 e_1 e 1 β and e 2 e_2 e 2 β , and
min β‘ u β U β₯ v β u β₯ = β₯ v β P U v β₯ = 1 + 1 + 0 = 2 . \min_{u \in U} \|v - u\| = \|v - P_U v\| = \sqrt{1 + 1 + 0} = \sqrt{2}. u β U min β β₯ v β u β₯ = β₯ v β P U β v β₯ = 1 + 1 + 0 β = 2 β .
Problem 2 Β· The Formula Needs an Orthonormal Basis
Given: In R 3 \mathbf{R}^3 R 3 with the dot product, U = span β‘ ( ( 1 , 1 , 0 ) , ( 1 , 0 , 0 ) ) U = \operatorname{span}\big((1, 1, 0), (1, 0, 0)\big) U = span ( ( 1 , 1 , 0 ) , ( 1 , 0 , 0 ) ) and v = ( 1 , 2 , 3 ) v = (1, 2, 3) v = ( 1 , 2 , 3 ) . Find the point of U U U closest to v v v .
a ( 4 , 3 , 0 ) (4, 3, 0) ( 4 , 3 , 0 )
b ( 1 , 2 , 0 ) (1, 2, 0) ( 1 , 2 , 0 )
c ( 3 2 , 3 2 , 0 ) \big(\tfrac{3}{2}, \tfrac{3}{2}, 0\big) ( 2 3 β , 2 3 β , 0 )
d ( 0 , 0 , 3 ) (0, 0, 3) ( 0 , 0 , 3 )
β
Correct! U U U is the
x y xy x y -plane, and GramβSchmidt gives the orthonormal basis
( 1 , 0 , 0 ) , ( 0 , 1 , 0 ) (1, 0, 0), (0, 1, 0) ( 1 , 0 , 0 ) , ( 0 , 1 , 0 ) , so
P U v = ( 1 , 2 , 0 ) P_U v = (1, 2, 0) P U β v = ( 1 , 2 , 0 ) .
β Close, butβ¦ β¨ v , w 1 β© w 1 + β¨ v , w 2 β© w 2 \langle v, w_1 \rangle w_1 + \langle v, w_2 \rangle w_2 β¨ v , w 1 β β© w 1 β + β¨ v , w 2 β β© w 2 β with
w 1 = ( 1 , 1 , 0 ) w_1 = (1, 1, 0) w 1 β = ( 1 , 1 , 0 ) ,
w 2 = ( 1 , 0 , 0 ) w_2 = (1, 0, 0) w 2 β = ( 1 , 0 , 0 ) uses a basis that is neither orthogonal nor normalized; run GramβSchmidt first.
β Not quite. ( 3 2 , 3 2 , 0 ) \big(\tfrac{3}{2}, \tfrac{3}{2}, 0\big) ( 2 3 β , 2 3 β , 0 ) is the projection onto the line spanned by
( 1 , 1 , 0 ) (1, 1, 0) ( 1 , 1 , 0 ) alone, a smaller subspace than
U U U .
β Not quite. ( 0 , 0 , 3 ) = v β P U v (0, 0, 3) = v - P_U v ( 0 , 0 , 3 ) = v β P U β v is the piece of
v v v in
U β₯ U^\perp U β₯ ; the closest point is the piece in
U U U .
Show solution
Run GramβSchmidt on w 1 = ( 1 , 1 , 0 ) w_1 = (1, 1, 0) w 1 β = ( 1 , 1 , 0 ) , w 2 = ( 1 , 0 , 0 ) w_2 = (1, 0, 0) w 2 β = ( 1 , 0 , 0 ) :
e 1 = 1 2 ( 1 , 1 , 0 ) , w 2 β β¨ w 2 , e 1 β© e 1 = ( 1 , 0 , 0 ) β 1 2 ( 1 , 1 , 0 ) = ( 1 2 , β 1 2 , 0 ) , e 2 = 1 2 ( 1 , β 1 , 0 ) . e_1 = \tfrac{1}{\sqrt{2}}(1, 1, 0), \qquad w_2 - \langle w_2, e_1 \rangle e_1 = (1, 0, 0) - \tfrac{1}{2}(1, 1, 0) = \big(\tfrac{1}{2}, -\tfrac{1}{2}, 0\big), \qquad e_2 = \tfrac{1}{\sqrt{2}}(1, -1, 0). e 1 β = 2 β 1 β ( 1 , 1 , 0 ) , w 2 β β β¨ w 2 β , e 1 β β© e 1 β = ( 1 , 0 , 0 ) β 2 1 β ( 1 , 1 , 0 ) = ( 2 1 β , β 2 1 β , 0 ) , e 2 β = 2 β 1 β ( 1 , β 1 , 0 ) .
Now apply the formula:
β¨ v , e 1 β© = 3 2 , β¨ v , e 2 β© = β 1 2 , P U v = 3 2 ( 1 , 1 , 0 ) β 1 2 ( 1 , β 1 , 0 ) = ( 1 , 2 , 0 ) . \langle v, e_1 \rangle = \tfrac{3}{\sqrt{2}}, \quad \langle v, e_2 \rangle = -\tfrac{1}{\sqrt{2}}, \quad P_U v = \tfrac{3}{2}(1, 1, 0) - \tfrac{1}{2}(1, -1, 0) = (1, 2, 0). β¨ v , e 1 β β© = 2 β 3 β , β¨ v , e 2 β β© = β 2 β 1 β , P U β v = 2 3 β ( 1 , 1 , 0 ) β 2 1 β ( 1 , β 1 , 0 ) = ( 1 , 2 , 0 ) .
Check: v β P U v = ( 0 , 0 , 3 ) v - P_U v = (0, 0, 3) v β P U β v = ( 0 , 0 , 3 ) is orthogonal to both ( 1 , 1 , 0 ) (1, 1, 0) ( 1 , 1 , 0 ) and ( 1 , 0 , 0 ) (1, 0, 0) ( 1 , 0 , 0 ) , so it lies in U β₯ U^\perp U β₯ , and the closest point is ( 1 , 2 , 0 ) (1, 2, 0) ( 1 , 2 , 0 ) at distance 3 3 3 .
Problem 3 Β· Best Line for Sine
Given: V = C [ β Ο , Ο ] V = C[-\pi, \pi] V = C [ β Ο , Ο ] with β¨ f , g β© = β« β Ο Ο f g \langle f, g \rangle = \int_{-\pi}^{\pi} f g β¨ f , g β© = β« β Ο Ο β f g , U = P 1 ( R ) U = \mathcal{P}_1(\mathbf{R}) U = P 1 β ( R ) , and v = sin β‘ v = \sin v = sin . You may use β« β Ο Ο x sin β‘ x β d x = 2 Ο \int_{-\pi}^{\pi} x \sin x \, dx = 2\pi β« β Ο Ο β x sin x d x = 2 Ο , β« β Ο Ο x 2 β d x = 2 Ο 3 3 \int_{-\pi}^{\pi} x^2 \, dx = \tfrac{2\pi^3}{3} β« β Ο Ο β x 2 d x = 3 2 Ο 3 β and β« β Ο Ο sin β‘ 2 x β d x = Ο \int_{-\pi}^{\pi} \sin^2 x \, dx = \pi β« β Ο Ο β sin 2 x d x = Ο . Find the closest point u = P U ( sin β‘ ) u = P_U(\sin) u = P U β ( sin ) and the minimum value of β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x \int_{-\pi}^{\pi} |\sin x - u(x)|^2 \, dx β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x .
What is P U ( sin β‘ ) P_U(\sin) P U β ( sin ) ?
a u ( x ) = x u(x) = x u ( x ) = x
b u ( x ) = 2 Ο x u(x) = 2\pi x u ( x ) = 2 Ο x
c u ( x ) = Ο 2 3 x u(x) = \tfrac{\pi^2}{3} x u ( x ) = 3 Ο 2 β x
d u ( x ) = 3 Ο 2 x u(x) = \tfrac{3}{\pi^2} x u ( x ) = Ο 2 3 β x
What is the minimum of β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x \int_{-\pi}^{\pi} |\sin x - u(x)|^2 \, dx β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x ?
a Ο \pi Ο
b 6 Ο \tfrac{6}{\pi} Ο 6 β
c Ο β 6 Ο \pi - \tfrac{6}{\pi} Ο β Ο 6 β
d Ο β 3 Ο 2 \pi - \tfrac{3}{\pi^2} Ο β Ο 2 3 β
β
Correct! P U ( sin β‘ ) = 3 Ο 2 x β 0.304 x P_U(\sin) = \tfrac{3}{\pi^2}x \approx 0.304x P U β ( sin ) = Ο 2 3 β x β 0.304 x , and the squared error is
Ο β 6 Ο β 1.2317 \pi - \tfrac{6}{\pi} \approx 1.2317 Ο β Ο 6 β β 1.2317 .
β Not quite. x x x is the degree-1 Taylor polynomial, which matches
sin β‘ \sin sin at
0 0 0 ; it is not the closest point of
U U U in the integral norm.
β Close, butβ¦ β¨ sin β‘ , x β© x \langle \sin, x \rangle x β¨ sin , x β© x forgets to divide by
β₯ x β₯ 2 = 2 Ο 3 3 \|x\|^2 = \tfrac{2\pi^3}{3} β₯ x β₯ 2 = 3 2 Ο 3 β ; the formula needs a unit vector.
β Not quite. The projection onto
span β‘ ( x ) \operatorname{span}(x) span ( x ) is
β¨ sin β‘ , x β© β₯ x β₯ 2 β x \tfrac{\langle \sin, x \rangle}{\|x\|^2}\, x β₯ x β₯ 2 β¨ s i n , x β© β x ; compute that ratio carefully.
β Not quite. By Pythagoras,
β₯ sin β‘ β P U sin β‘ β₯ 2 = β₯ sin β‘ β₯ 2 β β¨ sin β‘ , e 2 β© 2 \|\sin - P_U \sin\|^2 = \|\sin\|^2 - \langle \sin, e_2 \rangle^2 β₯ sin β P U β sin β₯ 2 = β₯ sin β₯ 2 β β¨ sin , e 2 β β© 2 , where
e 2 = x / β₯ x β₯ e_2 = x / \|x\| e 2 β = x /β₯ x β₯ .
Show solution
Orthonormal basis of U U U . On the symmetric interval β¨ 1 , x β© = 0 \langle 1, x \rangle = 0 β¨ 1 , x β© = 0 , so GramβSchmidt only normalizes: e 1 = 1 2 Ο e_1 = \tfrac{1}{\sqrt{2\pi}} e 1 β = 2 Ο β 1 β and e 2 = x / 2 Ο 3 / 3 e_2 = x \big/ \sqrt{2\pi^3/3} e 2 β = x / 2 Ο 3 /3 β .
Coefficients. β¨ sin β‘ , e 1 β© = 0 \langle \sin, e_1 \rangle = 0 β¨ sin , e 1 β β© = 0 because sin β‘ \sin sin is odd. Then
P U ( sin β‘ ) = β¨ sin β‘ , e 2 β© e 2 = β¨ sin β‘ , x β© β₯ x β₯ 2 β x = 2 Ο 2 Ο 3 / 3 β x = 3 Ο 2 β x β 0.304 x . P_U(\sin) = \langle \sin, e_2 \rangle e_2 = \frac{\langle \sin, x \rangle}{\|x\|^2}\, x = \frac{2\pi}{2\pi^3/3}\, x = \frac{3}{\pi^2}\, x \approx 0.304x. P U β ( sin ) = β¨ sin , e 2 β β© e 2 β = β₯ x β₯ 2 β¨ sin , x β© β x = 2 Ο 3 /3 2 Ο β x = Ο 2 3 β x β 0.304 x .
Minimum squared error. Since sin β‘ = P U ( sin β‘ ) + ( sin β‘ β P U sin β‘ ) \sin = P_U(\sin) + (\sin - P_U \sin) sin = P U β ( sin ) + ( sin β P U β sin ) with orthogonal pieces,
β₯ sin β‘ β P U sin β‘ β₯ 2 = β₯ sin β‘ β₯ 2 β β¨ sin β‘ , e 2 β© 2 = Ο β ( 2 Ο ) 2 2 Ο 3 / 3 = Ο β 6 Ο β 1.2317. \|\sin - P_U \sin\|^2 = \|\sin\|^2 - \langle \sin, e_2 \rangle^2 = \pi - \frac{(2\pi)^2}{2\pi^3/3} = \pi - \frac{6}{\pi} \approx 1.2317. β₯ sin β P U β sin β₯ 2 = β₯ sin β₯ 2 β β¨ sin , e 2 β β© 2 = Ο β 2 Ο 3 /3 ( 2 Ο ) 2 β = Ο β Ο 6 β β 1.2317.
Problem 4 Β· What the Theorem Guarantees
Given: U = P 5 ( R ) β C [ β Ο , Ο ] U = \mathcal{P}_5(\mathbf{R}) \subseteq C[-\pi, \pi] U = P 5 β ( R ) β C [ β Ο , Ο ] with the integral inner product, u = P U ( sin β‘ ) u = P_U(\sin) u = P U β ( sin ) , and the Taylor polynomial p ( x ) = x β x 3 3 ! + x 5 5 ! p(x) = x - \tfrac{x^3}{3!} + \tfrac{x^5}{5!} p ( x ) = x β 3 ! x 3 β + 5 ! x 5 β , which lies in U U U and is not equal to u u u . Which statement follows from the theorem?
a β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x < β« β Ο Ο β£ sin β‘ x β p ( x ) β£ 2 β d x \int_{-\pi}^{\pi} |\sin x - u(x)|^2\,dx \lt \int_{-\pi}^{\pi} |\sin x - p(x)|^2\,dx β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x < β« β Ο Ο β β£ sin x β p ( x ) β£ 2 d x
b β£ sin β‘ x β u ( x ) β£ β€ β£ sin β‘ x β p ( x ) β£ |\sin x - u(x)| \le |\sin x - p(x)| β£ sin x β u ( x ) β£ β€ β£ sin x β p ( x ) β£ for every x β [ β Ο , Ο ] x \in [-\pi, \pi] x β [ β Ο , Ο ]
c β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x = β« β Ο Ο β£ sin β‘ x β p ( x ) β£ 2 β d x \int_{-\pi}^{\pi} |\sin x - u(x)|^2\,dx = \int_{-\pi}^{\pi} |\sin x - p(x)|^2\,dx β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x = β« β Ο Ο β β£ sin x β p ( x ) β£ 2 d x , since both have degree 5 5 5
d Nothing, because C [ β Ο , Ο ] C[-\pi, \pi] C [ β Ο , Ο ] is infinite-dimensional
β
Correct! The inequality
β₯ v β P U v β₯ β€ β₯ v β p β₯ \|v - P_U v\| \le \|v - p\| β₯ v β P U β v β₯ β€ β₯ v β p β₯ is strict because equality would force
p = P U v p = P_U v p = P U β v ; numerically the two integrals are about
0.000116 0.000116 0.000116 and
0.119 0.119 0.119 .
β Not quite. The theorem compares norms, and this norm is an integral. At
x = 0.5 x = 0.5 x = 0.5 the Taylor error is about
0.0000015 0.0000015 0.0000015 while
β£ sin β‘ 0.5 β u ( 0.5 ) β£ β 0.0047 |\sin 0.5 - u(0.5)| \approx 0.0047 β£ sin 0.5 β u ( 0.5 ) β£ β 0.0047 .
β Not quite. Equality in the theorem holds only when the competitor is
P U v P_U v P U β v itself, and
p β u p \ne u p ξ = u .
β Not quite. The hypothesis is that
U U U is finite-dimensional, which
P 5 ( R ) \mathcal{P}_5(\mathbf{R}) P 5 β ( R ) is (
dim β‘ U = 6 \dim U = 6 dim U = 6 );
V V V may be infinite-dimensional.
Show solution
The theorem applies because U = P 5 ( R ) U = \mathcal{P}_5(\mathbf{R}) U = P 5 β ( R ) is finite-dimensional, and p β U p \in U p β U . It gives β₯ sin β‘ β u β₯ β€ β₯ sin β‘ β p β₯ \|\sin - u\| \le \|\sin - p\| β₯ sin β u β₯ β€ β₯ sin β p β₯ , with equality iff p = u p = u p = u . Since p β u p \ne u p ξ = u , the inequality is strict, and squaring the norms gives
β« β Ο Ο β£ sin β‘ x β u ( x ) β£ 2 β d x < β« β Ο Ο β£ sin β‘ x β p ( x ) β£ 2 β d x . \int_{-\pi}^{\pi} |\sin x - u(x)|^2\,dx \lt \int_{-\pi}^{\pi} |\sin x - p(x)|^2\,dx. β« β Ο Ο β β£ sin x β u ( x ) β£ 2 d x < β« β Ο Ο β β£ sin x β p ( x ) β£ 2 d x .
Numerically the left side is about 0.000116 0.000116 0.000116 and the right side about 0.119 0.119 0.119 . The theorem says nothing about single points: for β£ x β£ |x| β£ x β£ below about 1.21 1.21 1.21 the Taylor polynomial is the closer of the two, while at x = 3 x = 3 x = 3 the error of u u u is about 0.0014 0.0014 0.0014 against 0.38 0.38 0.38 for p p p , a fact we checked, not one the theorem promises.
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