Systems Theory

Field

Field

A field is a set \( \mathbb{F} \) with two binary operators, addition \((+)\) and multiplication \((\cdot)\), defined on the set \(S\). The binary operators satisfy the following axioms:

  1. Additive associativity \[(\alpha + \beta) + \gamma = \alpha + (\beta + \gamma)\] \[(\alpha \cdot \beta) \cdot \gamma = \alpha \cdot (\beta \cdot \gamma)\]
  2. Commutativity \[\alpha + \beta = \beta + \alpha\] \[\alpha \cdot \beta = \beta \cdot \alpha\]
  3. Additive identity: \(\exists\) a distinct element \(0\in S\) s.t. \[\alpha + 0 = \alpha = 0 + \alpha\]
  4. Multiplicative identity: \(\exists\) a distinct element \(1\in S\) s.t. \[\alpha \cdot 1 = \alpha = \alpha\]
  5. Additive inverse \[\forall \alpha \in S, \exists (-\alpha) \text{ s.t. } \alpha + (-\alpha) = 0\]
  6. Distributivity \[\alpha \cdot (\beta + \gamma) = (\alpha \cdot \beta) + (\alpha \cdot \gamma)\]
  7. Multiplicative inverse\[\forall \alpha \neq 0 \in S, \exists \alpha^{-1} \text{ s.t. } \alpha \cdot \alpha^{-1} = 1\]
Examples

Vector space

Vector Space

Vector space over a field \(\mathbb{F}\) is a non-empty set \(V\) with a vector addition \((+)\) and a scalar multiplication \((\cdot)\):

  1. Vector addition (+): \( V \times V \to V \)
  2. Scalar multiplication (·): \( \mathbb{F} \times V \to V \)

Vector addition and scalar multiplication satisfy the following axioms:

  1. Associativity: \[ (x + y) + z = x + (y + z) \]
  2. Commutativity: \[ x + y = y + x \]
  3. Identity: \( \exists 0 \in V \) such that \[ x + 0 = 0 + x = x \]
  4. Inverse: \( \forall x \in V, \exists (-x) \in V \) such that \[ x + (-x) = 0 \]
  5. Distributivity of scalar multiplication over vector addition: \[ \alpha \cdot (x + y) = \alpha \cdot x + \alpha \cdot y \]
  6. Distributivity of scalar multiplication over field addition: \[ (\alpha + \beta) \cdot x = \alpha \cdot x + \beta \cdot x \]
  7. Compatibility of scalar multiplication: \[ (\alpha \times \beta) \cdot v = \alpha \cdot (\beta \cdot v) \]
  8. Identity of scalar multiplication: \[ 1 \cdot v = v \] where \( 1 \) is the multiplicative identity in \( F \)
Examples
Linearly independent set of vectors

A set of vectors \( M = \{x_1, \ldots, x_p\} \) are linearly independent if:

\[ \sum_{i=1}^p \alpha_i x_i = 0 \Rightarrow \alpha_i = 0 \quad \forall i \]
Span of a set of vectors

For \( M = \{x_1, \ldots, x_p\} \), the span is:

\[ \text{span}(M) = \left\{ z \in V : z = \sum_{i=1}^p \alpha_i x_i, \alpha_i \in \mathbb{F} \right\} \]

Basis of a vector space

A set \( M = \{x_1, \ldots, x_p\} \) is a basis for the vector space \( V \) if:

  1. \( M \) is linearly independent
  2. Every \( z \in V \) can be written as \( z = \sum_{i=1}^p \alpha_i x_i \)
Dimension of a vector space

The dimension of a vector space is the number of elements in its basis.

Isomorphism

Two vector spaces \( V_{\mathbb{F}} \) and \( W_{\mathbb{F}} \) are isomorphic if there exists a bijective mapping \(V_\mathbb{F} \mapsto W_\mathbb{F}\) that preserves vector addition and scalar multiplication: \[ \alpha_1 x_1 + \alpha_2 x_2 \mapsto \alpha_1 y_1 + \alpha_2 y_2 \]

Example

Set of functions and their fourier transforms form an isomorphism.

Subspace

A subset \( S \subseteq V \) is called a subspace if for every \( x,y \in S \) and \( \alpha, \beta \in F \):

\[ \alpha x + \beta y \in S \]

A subspace of a vector space is also a vector space.

Dual space

Linear functional

A linear functional \(\phi\) on a vector space \(V\) is a mapping \(\phi:V\rightarrow \mathbb{F}\) that satisfies: \[ \phi(\alpha v_1+\beta v_2) = \alpha \phi(v_1) + \beta \phi(v_2) \] Here, \(\alpha,\beta\in\mathbb{F}\), and \(v_1,v_2\in V\)

Dual space

Dual space \(V^\prime\) of a vector space \(V\) is the set of all linear functionals on \(V\).

Example
Dual vector space

Set of all linear functional forms a vector space.

Basis for dual space

Let \( \{x_1, \ldots, x_n\} \) be a basis for \( V \). A dual basis \( \{y_1, \ldots, y_n\} \) is given by:

\[ y_i(x_j) = \delta_{ij} = \begin{cases} 1 & \text{if } i = j \\ 0 & \text{if } i \neq j \end{cases} \]

For any \( y \in V^\prime \):

\[ y(x) = \sum_{i=1}^n y(x_i) y_i(x) = \sum_{i=1}^n \alpha_i y_i(x) \]
Direct sum

For subspaces \(M, N \subset V\), direct sum \(V = M \oplus N\) means every \(x \in V\) can be written uniquely as:

\[ x = z + t \quad \text{where } z \in M, t \in N \]
Annihilators

For a subspace \( M \subseteq V \), its annihilator \( M^\circ \) is given by:

\[ M^\circ = \{ y \in V^\prime \mid y(x) = 0 \ \forall x \in M \} \]

Properties of Annihilators

  1. \( M^\circ \) is a subspace of \( V^\prime \)
  2. If \( y_1, y_2 \in M^\circ \), then \( \alpha_1 y_1 + \alpha_2 y_2 \in M^\circ \): \[ (\alpha_1 y_1 + \alpha_2 y_2)(x) = \alpha_1 y_1(x) + \alpha_2 y_2(x) = 0 \quad \forall x \in M \]
Example

For \( M = \text{span}\left\{ \begin{pmatrix}1\\2\\3\end{pmatrix} \right\} \subset \mathbb{R}^3\):

\[ M^\circ = \left\{ y \in (\mathbb{R}^3)^* \mid y_1 + 2y_2 + 3y_3 = 0 \right\} \]

A basis for \( M^\circ \) could be:

\[ \left\{ \begin{pmatrix}2\\-1\\0\end{pmatrix}, \begin{pmatrix}3\\0\\-1\end{pmatrix} \right\} \]

Thus \( \dim(M^\circ) = 2 \) (a 2D subspace of \( V^\prime \)).

Fundamental dimension theorem

For any subspace \( M \subseteq V \):

\[ \dim(M) + \dim(M^\circ) = \dim(V) \]

Scanned notes

These scanned lecture notes are from the course SC 625 (Systems Theory) at Indian Institute of Technology, Bombay. Use them at your own discretion. If you would like to help digitize these lecture notes, contact the editor.

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Author

Anurag Gupta is an M.S. graduate in Electrical and Computer Engineering from Cornell University. He also holds an M.Tech degree in Systems and Control Engineering and a B.Tech degree in Electrical Engineering from the Indian Institute of Technology, Bombay.


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