- Source: Parallelogram law
In mathematics, the simplest form of the parallelogram law (also called the parallelogram identity) belongs to elementary geometry. It states that the sum of the squares of the lengths of the four sides of a parallelogram equals the sum of the squares of the lengths of the two diagonals. We use these notations for the sides: AB, BC, CD, DA. But since in Euclidean geometry a parallelogram necessarily has opposite sides equal, that is, AB = CD and BC = DA, the law can be stated as
2
A
B
2
+
2
B
C
2
=
A
C
2
+
B
D
2
{\displaystyle 2AB^{2}+2BC^{2}=AC^{2}+BD^{2}\,}
If the parallelogram is a rectangle, the two diagonals are of equal lengths AC = BD, so
2
A
B
2
+
2
B
C
2
=
2
A
C
2
{\displaystyle 2AB^{2}+2BC^{2}=2AC^{2}}
and the statement reduces to the Pythagorean theorem. For the general quadrilateral (with four sides not necessarily equal) Euler's quadrilateral theorem states
A
B
2
+
B
C
2
+
C
D
2
+
D
A
2
=
A
C
2
+
B
D
2
+
4
x
2
,
{\displaystyle AB^{2}+BC^{2}+CD^{2}+DA^{2}=AC^{2}+BD^{2}+4x^{2},}
where
x
{\displaystyle x}
is the length of the line segment joining the midpoints of the diagonals. It can be seen from the diagram that
x
=
0
{\displaystyle x=0}
for a parallelogram, and so the general formula simplifies to the parallelogram law.
Proof
In the parallelogram on the right, let AD = BC = a, AB = DC = b,
∠
B
A
D
=
α
.
{\displaystyle \angle BAD=\alpha .}
By using the law of cosines in triangle
△
B
A
D
,
{\displaystyle \triangle BAD,}
we get:
a
2
+
b
2
−
2
a
b
cos
(
α
)
=
B
D
2
.
{\displaystyle a^{2}+b^{2}-2ab\cos(\alpha )=BD^{2}.}
In a parallelogram, adjacent angles are supplementary, therefore
∠
A
D
C
=
180
∘
−
α
.
{\displaystyle \angle ADC=180^{\circ }-\alpha .}
Using the law of cosines in triangle
△
A
D
C
,
{\displaystyle \triangle ADC,}
produces:
a
2
+
b
2
−
2
a
b
cos
(
180
∘
−
α
)
=
A
C
2
.
{\displaystyle a^{2}+b^{2}-2ab\cos(180^{\circ }-\alpha )=AC^{2}.}
By applying the trigonometric identity
cos
(
180
∘
−
x
)
=
−
cos
x
{\displaystyle \cos(180^{\circ }-x)=-\cos x}
to the former result proves:
a
2
+
b
2
+
2
a
b
cos
(
α
)
=
A
C
2
.
{\displaystyle a^{2}+b^{2}+2ab\cos(\alpha )=AC^{2}.}
Now the sum of squares
B
D
2
+
A
C
2
{\displaystyle BD^{2}+AC^{2}}
can be expressed as:
B
D
2
+
A
C
2
=
a
2
+
b
2
−
2
a
b
cos
(
α
)
+
a
2
+
b
2
+
2
a
b
cos
(
α
)
.
{\displaystyle BD^{2}+AC^{2}=a^{2}+b^{2}-2ab\cos(\alpha )+a^{2}+b^{2}+2ab\cos(\alpha ).}
Simplifying this expression, it becomes:
B
D
2
+
A
C
2
=
2
a
2
+
2
b
2
.
{\displaystyle BD^{2}+AC^{2}=2a^{2}+2b^{2}.}
The parallelogram law in inner product spaces
In a normed space, the statement of the parallelogram law is an equation relating norms:
2
‖
x
‖
2
+
2
‖
y
‖
2
=
‖
x
+
y
‖
2
+
‖
x
−
y
‖
2
for all
x
,
y
.
{\displaystyle 2\|x\|^{2}+2\|y\|^{2}=\|x+y\|^{2}+\|x-y\|^{2}\quad {\text{ for all }}x,y.}
The parallelogram law is equivalent to the seemingly weaker statement:
2
‖
x
‖
2
+
2
‖
y
‖
2
≤
‖
x
+
y
‖
2
+
‖
x
−
y
‖
2
for all
x
,
y
{\displaystyle 2\|x\|^{2}+2\|y\|^{2}\leq \|x+y\|^{2}+\|x-y\|^{2}\quad {\text{ for all }}x,y}
because the reverse inequality can be obtained from it by substituting
1
2
(
x
+
y
)
{\textstyle {\frac {1}{2}}\left(x+y\right)}
for
x
,
{\displaystyle x,}
and
1
2
(
x
−
y
)
{\textstyle {\frac {1}{2}}\left(x-y\right)}
for
y
,
{\displaystyle y,}
and then simplifying. With the same proof, the parallelogram law is also equivalent to:
‖
x
+
y
‖
2
+
‖
x
−
y
‖
2
≤
2
‖
x
‖
2
+
2
‖
y
‖
2
for all
x
,
y
.
{\displaystyle \|x+y\|^{2}+\|x-y\|^{2}\leq 2\|x\|^{2}+2\|y\|^{2}\quad {\text{ for all }}x,y.}
In an inner product space, the norm is determined using the inner product:
‖
x
‖
2
=
⟨
x
,
x
⟩
.
{\displaystyle \|x\|^{2}=\langle x,x\rangle .}
As a consequence of this definition, in an inner product space the parallelogram law is an algebraic identity, readily established using the properties of the inner product:
‖
x
+
y
‖
2
=
⟨
x
+
y
,
x
+
y
⟩
=
⟨
x
,
x
⟩
+
⟨
x
,
y
⟩
+
⟨
y
,
x
⟩
+
⟨
y
,
y
⟩
,
{\displaystyle \|x+y\|^{2}=\langle x+y,x+y\rangle =\langle x,x\rangle +\langle x,y\rangle +\langle y,x\rangle +\langle y,y\rangle ,}
‖
x
−
y
‖
2
=
⟨
x
−
y
,
x
−
y
⟩
=
⟨
x
,
x
⟩
−
⟨
x
,
y
⟩
−
⟨
y
,
x
⟩
+
⟨
y
,
y
⟩
.
{\displaystyle \|x-y\|^{2}=\langle x-y,x-y\rangle =\langle x,x\rangle -\langle x,y\rangle -\langle y,x\rangle +\langle y,y\rangle .}
Adding these two expressions:
‖
x
+
y
‖
2
+
‖
x
−
y
‖
2
=
2
⟨
x
,
x
⟩
+
2
⟨
y
,
y
⟩
=
2
‖
x
‖
2
+
2
‖
y
‖
2
,
{\displaystyle \|x+y\|^{2}+\|x-y\|^{2}=2\langle x,x\rangle +2\langle y,y\rangle =2\|x\|^{2}+2\|y\|^{2},}
as required.
If
x
{\displaystyle x}
is orthogonal to
y
,
{\displaystyle y,}
meaning
⟨
x
,
y
⟩
=
0
,
{\displaystyle \langle x,\ y\rangle =0,}
and the above equation for the norm of a sum becomes:
‖
x
+
y
‖
2
=
⟨
x
,
x
⟩
+
⟨
x
,
y
⟩
+
⟨
y
,
x
⟩
+
⟨
y
,
y
⟩
=
‖
x
‖
2
+
‖
y
‖
2
,
{\displaystyle \|x+y\|^{2}=\langle x,x\rangle +\langle x,y\rangle +\langle y,x\rangle +\langle y,y\rangle =\|x\|^{2}+\|y\|^{2},}
which is Pythagoras' theorem.
Normed vector spaces satisfying the parallelogram law
Most real and complex normed vector spaces do not have inner products, but all normed vector spaces have norms (by definition). For example, a commonly used norm for a vector
x
=
(
x
1
,
x
2
,
…
,
x
n
)
{\displaystyle x=(x_{1},x_{2},\ldots ,x_{n})}
in the real coordinate space
R
n
{\displaystyle \mathbb {R} ^{n}}
is the
p
{\displaystyle p}
-norm:
‖
x
‖
p
=
(
|
x
1
|
p
+
|
x
2
|
p
+
⋯
+
|
x
n
|
p
)
1
/
p
.
{\displaystyle \|x\|_{p}=\left(|x_{1}|^{p}+|x_{2}|^{p}+\dotsb +|x_{n}|^{p}\right)^{1/p}.}
Given a norm, one can evaluate both sides of the parallelogram law above. A remarkable fact is that if the parallelogram law holds, then the norm must arise in the usual way from some inner product. In particular, it holds for the
p
{\displaystyle p}
-norm if and only if
p
=
2
,
{\displaystyle p=2,}
the so-called Euclidean norm or standard norm.
For any norm satisfying the parallelogram law (which necessarily is an inner product norm), the inner product generating the norm is unique as a consequence of the polarization identity. In the real case, the polarization identity is given by:
⟨
x
,
y
⟩
=
‖
x
+
y
‖
2
−
‖
x
−
y
‖
2
4
,
{\displaystyle \langle x,y\rangle ={\frac {\|x+y\|^{2}-\|x-y\|^{2}}{4}},}
or equivalently by
‖
x
+
y
‖
2
−
‖
x
‖
2
−
‖
y
‖
2
2
or
‖
x
‖
2
+
‖
y
‖
2
−
‖
x
−
y
‖
2
2
.
{\displaystyle {\frac {\|x+y\|^{2}-\|x\|^{2}-\|y\|^{2}}{2}}\qquad {\text{ or }}\qquad {\frac {\|x\|^{2}+\|y\|^{2}-\|x-y\|^{2}}{2}}.}
In the complex case it is given by:
⟨
x
,
y
⟩
=
‖
x
+
y
‖
2
−
‖
x
−
y
‖
2
4
+
i
‖
i
x
−
y
‖
2
−
‖
i
x
+
y
‖
2
4
.
{\displaystyle \langle x,y\rangle ={\frac {\|x+y\|^{2}-\|x-y\|^{2}}{4}}+i{\frac {\|ix-y\|^{2}-\|ix+y\|^{2}}{4}}.}
For example, using the
p
{\displaystyle p}
-norm with
p
=
2
{\displaystyle p=2}
and real vectors
x
{\displaystyle x}
and
y
,
{\displaystyle y,}
the evaluation of the inner product proceeds as follows:
⟨
x
,
y
⟩
=
‖
x
+
y
‖
2
−
‖
x
−
y
‖
2
4
=
1
4
(
∑
i
|
x
i
+
y
i
|
2
−
∑
i
|
x
i
−
y
i
|
2
)
=
1
4
(
4
∑
i
x
i
y
i
)
=
x
⋅
y
,
{\displaystyle {\begin{aligned}\langle x,y\rangle &={\frac {\|x+y\|^{2}-\|x-y\|^{2}}{4}}\\[4mu]&={\tfrac {1}{4}}\left(\sum _{i}|x_{i}+y_{i}|^{2}-\sum _{i}|x_{i}-y_{i}|^{2}\right)\\[2mu]&={\tfrac {1}{4}}\left(4\sum _{i}x_{i}y_{i}\right)\\&=x\cdot y,\\\end{aligned}}}
which is the standard dot product of two vectors.
Another necessary and sufficient condition for there to exist an inner product that induces the given norm
‖
⋅
‖
{\displaystyle \|\cdot \|}
is for the norm to satisfy Ptolemy's inequality:
‖
x
−
y
‖
‖
z
‖
+
‖
y
−
z
‖
‖
x
‖
≥
‖
x
−
z
‖
‖
y
‖
for all vectors
x
,
y
,
z
.
{\displaystyle \|x-y\|\,\|z\|~+~\|y-z\|\,\|x\|~\geq ~\|x-z\|\,\|y\|\qquad {\text{ for all vectors }}x,y,z.}
See also
Commutative property – Property of some mathematical operations
François Daviet – Royal Sardinian Army officer and mathematician (1734–1798)
Inner product space – Generalization of the dot product; used to define Hilbert spaces
Minkowski distance – Mathematical metric in normed vector space
Normed vector space – Vector space on which a distance is defined
Polarization identity – Formula relating the norm and the inner product in a inner product space
Ptolemy's inequality – inequality relating the six distances between four points on a planePages displaying wikidata descriptions as a fallback
References
External links
Weisstein, Eric W. "Parallelogram Law". MathWorld.
The Parallelogram Law Proven Simply at Dreamshire blog
The Parallelogram Law: A Proof Without Words at cut-the-knot
Kata Kunci Pencarian:
- Hukum jajaran genjang
- Dinasti Song
- Parallelogram law
- Parallelogram
- Rhombus
- Quadrilateral
- Polarization identity
- Hilbert space
- Pythagorean theorem
- Pseudo-Euclidean space
- Varignon's theorem
- Euler's quadrilateral theorem
