2025-04-27

1093: For Vectors Space and 2 Subspaces, if Sum of Projections into Subspaces Is Projection into Subspace, 2 Subspaces Are Perpendicular to Each Other w.r.t. Projections

<The previous article in this series | The table of contents of this series | The next article in this series>

description/proof of that for vectors space and 2 subspaces, if sum of projections into subspaces is projection into subspace, 2 subspaces are perpendicular to each other w.r.t. projections

Topics


About: vectors space

The table of contents of this article


Starting Context



Target Context


  • The reader will have a description and a proof of the proposition that for any vectors space and any 2 subspaces, if the sum of any projections into the subspaces is any projection into any another subspace, the 2 subspaces are perpendicular to each other with respect to the projections.

Orientation


There is a list of definitions discussed so far in this site.

There is a list of propositions discussed so far in this site.


Main Body


1: Structured Description


Here is the rules of Structured Description.

Entities:
F: { the fields }
V: { the F vectors spaces }
V1: { the vectors subspaces of V}
V2: { the vectors subspaces of V}
V3: { the vectors subspaces of V}
f1: :VV1, { the projections }
f2: :VV2, { the projections }
f3: :VV3, { the projections }
//

Statements:
f1+f2=f3

v1V1(f2(v1)=0)v2V2(f1(v2)=0)
//


2: Note


f1, f2, and f3 are defined somewhat independently according to the definition of projection from vectors space into vectors subspace, but as far as they satisfies the definition and f1+f2=f3 is satisfied, this proposition holds as Proof shows.

Typically, f1, f2, and f3 are defined uniformly according to the definition of orthogonal projection from vectors space with inner product into vectors subspace, and this proposition holds as a special case.


3: Proof


Whole Strategy: Step 1: do f3(f1+f2)(v1)=f3f3(v1) and see that f1f2(v1)+f2(v1)=0; Step 2: see that V1V2={0}; Step 3: see that f2(v1)=0; Step 4: conclude the proposition.

Step 1:

As f1+f2=f3, f3(f1+f2)=f3f3=f3.

Let v1V1 be any.

f3(f1+f2)(v1)=f3(v1).

f3(f1+f2)(v1)=f3(f1(v1)+f2(v1))=f3(v1+f2(v1))=f3(v1)+f3f2(v1).

So, f3(v1)+f3f2(v1)=f3(v1), which implies that f3f2(v1)=0.

(f1+f2)f2(v1)=0, so, f1f2(v1)+f2f2(v1)=f1f2(v1)+f2(v1)=0.

Step 2:

Let us see that V1V2={0}.

Let vV1V2 be any.

As f1+f2=f3, (f1+f2)(v)=f3(v).

But (f1+f2)(v)=f1(v)+f2(v)=v+v=2v.

So, f3(v)=2v.

f3f3(v)=f3(2v), which implies that f3(v)=2f3(v), so, 0=f3(v)f3(v)=2f3(v)f3(v)=f3(v). But as f3(v)=2v, 2v=0, so, v=0/2=0.

That means that V1V2={0}.

Step 3:

By Step 1, f1f2(v1)=f2(v1).

But the left hand side is in V1 and the right hand side is in V2, so, the both hand sides are in V1V2.

But by Step 2, V1V2={0}, and f2(v1)=0, which implies that f2(v1)=0.

Step 4:

By symmetry, for each v2V2, f1(v2)=0.


References


<The previous article in this series | The table of contents of this series | The next article in this series>