06-240/Classnotes For Thursday, September 21: Difference between revisions
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#<math> \forall x\; \exists\ y \ s.t.\ x+y=0 \ </math> |
#<math> \forall x\; \exists\ y \ s.t.\ x+y=0 \ </math> |
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#<math> 1.x=x \ </math> |
#<math> 1.x=x \ </math> |
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#<math> a(bx=(ab)x \ </math> |
#<math> a(bx)=(ab)x \ </math> |
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#<math> a(x+y)=ax+ay \ </math> |
#<math> a(x+y)=ax+ay \ </math> |
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#<math> (a+b)x=ax+bx \ </math> |
#<math> (a+b)x=ax+bx \ </math> |
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====''Examples''==== |
====''Examples''==== |
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'''Ex.1.''' |
'''Ex.1.''' |
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<math> F^n= \ |
<math> F^n= \lbrace(a_1,a_2,a_3,...,a_{n-1},a_n):\forall i\ a_i \in F \rbrace </math> <br/> |
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<math> n \in \mathbb{Z}\ , n \ge 0 </math> <br/> |
<math> n \in \mathbb{Z}\ , n \ge 0 </math> <br/> |
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<math> x=(a_1,...,a_2)\ y=(b_1,...,b_2)\ </math> <br/> |
<math> x=(a_1,...,a_2)\ y=(b_1,...,b_2)\ </math> <br/> |
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<math> a\in F\ ax=(aa_1,aa_2,...,aa_n) </math> <br/> |
<math> a\in F\ ax=(aa_1,aa_2,...,aa_n) </math> <br/> |
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<math> In \ \mathbb{Q}^3 \ ( \frac{3}{2},-2,7)+( \frac{-3}{2}, \frac{1}{3},240)=(0, \frac{-5}{3},247) </math> <br/> |
<math> In \ \mathbb{Q}^3 \ ( \frac{3}{2},-2,7)+( \frac{-3}{2}, \frac{1}{3},240)=(0, \frac{-5}{3},247) </math> <br/> |
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<math> 7( \frac{1}{5},\frac{1}{7},\frac{1}{9})=( \frac{7}{5},1,\frac{7}{9}) </math> <br/> |
<math> 7\left( \frac{1}{5},\frac{1}{7},\frac{1}{9}\right)=\left( \frac{7}{5},1,\frac{7}{9}\right) </math> <br/> |
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'''Ex.2.''' |
'''Ex.2.''' |
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<math> V=M_{m |
<math> V=M_{m\times n}(F)=\lbrace\begin{pmatrix} a_{11} & \cdots & a_{1n} \\ \vdots & |
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& \vdots \\ a_{m1} & \cdots & a_{mn}\end{pmatrix}: a_{ij} \in F \ |
& \vdots \\ a_{m1} & \cdots & a_{mn}\end{pmatrix}: a_{ij} \in F \rbrace </math> <br/> |
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<math> M_{3\times 2}( \mathbb{R})\ni \begin{pmatrix} 7 & -7 \\ \pi & \mathit{e} \\ -5 & 2 \end{pmatrix} </math> <br/> |
<math> M_{3\times 2}( \mathbb{R})\ni \begin{pmatrix} 7 & -7 \\ \pi & \mathit{e} \\ -5 & 2 \end{pmatrix} </math> <br/> |
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Addition by adding entry by entry: |
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<math> c\cdot M_{2\times 2}\ \begin{pmatrix} a_{11} & a_{12} \\ a_{21} & a_{22} \end{pmatrix}=\begin{pmatrix} c\cdot a_{11} & c\cdot a_{12} \\ c\cdot a_{21} & c\cdot a_{22} \end{pmatrix}</math> <br/> <br/> |
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Zero matrix has all entries = 0: |
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<math> 0_{M_{m\times n}}=\begin{pmatrix} 0 & \cdots & 0 \\ \vdots & |
<math> 0_{M_{m\times n}}=\begin{pmatrix} 0 & \cdots & 0 \\ \vdots & |
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& \vdots \\ 0 & \cdots & 0\end{pmatrix} </math> <br/> |
& \vdots \\ 0 & \cdots & 0\end{pmatrix} </math> <br/> |
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<math> f,g \in \mathcal{F}(S,\mathbb{R}) </math> <br/> |
<math> f,g \in \mathcal{F}(S,\mathbb{R}) </math> <br/> |
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<math> (f+g)(t)=f(t)+g(t)\ for\ any\ t\in S </math> <br/> |
<math> (f+g)(t)=f(t)+g(t)\ for\ any\ t\in S </math> <br/> |
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<math> (af)(t)=a |
<math> (af)(t)=a\cdot f(t)\ </math> |
Revision as of 09:42, 26 September 2006
A force has a direction & a magnitude.
Force Vectors
- There is a special force vector called 0.
- They can be added.
- They can be multiplied by any scalar.
====Properties==== (convention: x,y,z-vectors; a,b,c-scalars)
=====Definition===== Let F be a field "of scalars". A vector space over F is a set V (of "vectors") along with two operations:
- , so that
9.
Examples
Ex.1.
Ex.2.
Addition by adding entry by entry:
Multiplication by multiplying scalar c to all entries by M.
Zero matrix has all entries = 0:
Ex.3.
form a vector space over .
Ex.4.
F is a vector space over itself.
Ex.5.
is a vector space over .
Ex.6.
Let S be a set. Let