The lecturer states that the representation is unique because, in the context of a direct sum W⊕W⊥=R4, there is only one way to split a given vector into a part belonging to W and a part belonging to W⊥. No other pair of vectors from these subspaces can sum to the same original vector.
Conditions: The ambient space is R4.; W and W⊥ are the specific subspaces defined on the board.; The equation W⊕W⊥=R4 holds.
The lecturer states that the representation is unique because, in the context of a direct sum W⊕W⊥=R4, there is only one way to split a given vector into a part belonging to W and a part belonging to W⊥. No other pair of vectors from these subspaces can sum to the same original vector.
Conditions: The ambient space is R4.; W and W⊥ are the specific subspaces defined on the board.; The equation W⊕W⊥=R4 holds.
The representation is unique because the direct sum W⊕W⊥=R4 implies that the intersection of W and W⊥ contains only the zero vector. Therefore, there is only one way to express any vector in R4 as the sum of a vector from W and a vector from W⊥.
Conditions: W and W⊥ are subspaces of R4.; W∩W⊥={0}.; The equation W⊕W⊥=R4 holds.
The representation is unique because the direct sum W⊕W⊥=R4 implies that the intersection of W and W⊥ contains only the zero vector. Therefore, there is only one way to express any vector in R4 as the sum of a vector from W and a vector from W⊥.
Conditions: W and W⊥ are subspaces of R4.; W∩W⊥={0}.; The equation W⊕W⊥=R4 holds.