The example defines a subspace W spanned by the first two standard basis vectors of R4, and its orthogonal complement W⊥ spanned by the last two standard basis vectors. Together, they form a direct sum that equals the entire space R4.
Conditions: The ambient space is R4.; The bases are taken as given on the board.
The example defines a subspace W spanned by the first two standard basis vectors of R4, and its orthogonal complement W⊥ spanned by the last two standard basis vectors. Together, they form a direct sum that equals the entire space R4.
Conditions: The ambient space is R4.; The bases are taken as given on the board.
To decompose a vector in R4, you separate its components based on the bases of W and W⊥. The part corresponding to the basis of W (the first two coordinates) forms a vector in W, and the part corresponding to the basis of W⊥ (the last two coordinates) forms a vector in W⊥.
Conditions: The ambient space is R4.; W has basis ⎩⎨⎧1000,0100⎭⎬⎫.; W⊥ has basis ⎩⎨⎧0010,0001⎭⎬⎫.; The target vector is given, e.g., 43−26.
To decompose a vector in R4, you separate its components based on the bases of W and W⊥. The part corresponding to the basis of W (the first two coordinates) forms a vector in W, and the part corresponding to the basis of W⊥ (the last two coordinates) forms a vector in W⊥.
Conditions: The ambient space is R4.; W has basis ⎩⎨⎧1000,0100⎭⎬⎫.; W⊥ has basis ⎩⎨⎧0010,0001⎭⎬⎫.; The target vector is given, e.g., 43−26.
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.
A general vector in R4 is decomposed by separating its coordinates into two blocks. The first two coordinates form a vector in W, and the last two coordinates form a vector in W⊥.
Conditions: The ambient space is R4.; W has basis ⎩⎨⎧1000,0100⎭⎬⎫.; W⊥ has basis ⎩⎨⎧0010,0001⎭⎬⎫.; The vector is represented as abcd with a,b,c,d∈R.
A general vector in R4 is decomposed by separating its coordinates into two blocks. The first two coordinates form a vector in W, and the last two coordinates form a vector in W⊥.
Conditions: The ambient space is R4.; W has basis ⎩⎨⎧1000,0100⎭⎬⎫.; W⊥ has basis ⎩⎨⎧0010,0001⎭⎬⎫.; The vector is represented as abcd with a,b,c,d∈R.