book:chap2:2.8_cartesian_coordinates
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book:chap2:2.8_cartesian_coordinates [2021/11/06 17:01] – created abril | book:chap2:2.8_cartesian_coordinates [2022/04/01 21:13] (current) – jv | ||
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+ | [[forcestorques|2. Balancing Forces and Torques]] | ||
+ | * [[ 2.1 Motivation and Outline| 2.1 Motivation and outline: forces are vectors ]] | ||
+ | * [[ 2.2 Sets| 2.2 Sets ]] | ||
+ | * [[ 2.3 Groups| 2.3 Groups ]] | ||
+ | * [[ 2.4 Fields| 2.4 Fields ]] | ||
+ | * [[ 2.5 Vector spaces| 2.5 Vector spaces ]] | ||
+ | * [[ 2.6 Physics application balancing forces| 2.6. Physics application: | ||
+ | * [[ 2.7 The inner product | 2.7 The inner product]] | ||
+ | * ** 2.8 Cartesian coordinates ** | ||
+ | * [[ 2.9 Cross products --- torques| 2.9 Cross products — torques ]] | ||
+ | * [[ 2.10 Worked example Calder' | ||
+ | * [[ 2.11 Problems| 2.11 Problems ]] | ||
+ | * [[ 2.12 Further reading| 2.12 Further reading ]] | ||
+ | |||
+ | ---- | ||
+ | |||
==== 2.8 Cartesian coordinates ===== | ==== 2.8 Cartesian coordinates ===== | ||
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<WRAP 120pt left # | <WRAP 120pt left # | ||
- | {{vector-2Dcoordinates_E.png}} Figure 2.14: Representation of the vector $\mathbf c$ in terms of the orthogonal unit vectors $(\mathbf e_1, \mathbf e_2)$. | + | {{vector-2Dcoordinates_E.png}} |
+ | |||
+ | Figure 2.14: Representation of the vector $\mathbf c$ in terms of the orthogonal unit vectors $(\mathbf e_1, \mathbf e_2)$. | ||
</ | </ | ||
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</ | </ | ||
- | < | + | < |
- | {{vector-2Dcoordinates2.png}} Representation of the vector $\mathbf c$ of [[# | + | {{vector-2Dcoordinates2.png}} |
+ | |||
+ | Representation of the vector $\mathbf c$ of [[# | ||
</ | </ | ||
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<wrap lo> | <wrap lo> | ||
For a given basis the representation in terms of coordinates is unique. | For a given basis the representation in terms of coordinates is unique. | ||
- | </ | + | </ |
//Proof.// | //Proof.// | ||
1. The coordinates $a_i$ of a vector $\mathbf a$ are explicitly given by $a_i = \langle a \mid \mathbf e_i\rangle$. | 1. The coordinates $a_i$ of a vector $\mathbf a$ are explicitly given by $a_i = \langle a \mid \mathbf e_i\rangle$. | ||
- | This provides unique numbers for a given basis set.\\ | + | This provides unique numbers for a given basis set. |
2. Assume now that two vectors $\mathbf a$ and $\mathbf b$ have the same coordinate representation. | 2. Assume now that two vectors $\mathbf a$ and $\mathbf b$ have the same coordinate representation. | ||
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==== 2.8.1 Self Test ==== | ==== 2.8.1 Self Test ==== | ||
- | <wrap # | + | <wrap # |
a) Mark the following points in a Cartesian coordinate system: | a) Mark the following points in a Cartesian coordinate system: | ||
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(0, \, 0) \quad (0, \, 3) \quad (2, \, 5) \quad (4, \, 3) \quad (4, \,0) | (0, \, 0) \quad (0, \, 3) \quad (2, \, 5) \quad (4, \, 3) \quad (4, \,0) | ||
\end{align*} | \end{align*} | ||
- | Add the points $(0, \, 0) \; (4, \, 3) \; (0, \, 3) \; (4, \, 0)$, and connect the points in the given order. What do you see?\\ | + | Add the points $(0, \, 0) \; (4, \, 3) \; (0, \, 3) \; (4, \, 0)$, and connect the points in the given order. What do you see? |
b) What do you find when drawing a line segment connecting the following points? | b) What do you find when drawing a line segment connecting the following points? | ||
\begin{align*} | \begin{align*} | ||
(0, \, 0) \quad (1, \, 4) \quad (2, \, 0) \quad (-1, \, 3) \quad (3, \, 3) \quad (0, \, 0) | (0, \, 0) \quad (1, \, 4) \quad (2, \, 0) \quad (-1, \, 3) \quad (3, \, 3) \quad (0, \, 0) | ||
- | \end{align*}\\ | + | \end{align*} |
- | <wrap # | + | <wrap # |
- | < | + | < |
{{02_scalarProduct.png}} | {{02_scalarProduct.png}} | ||
</ | </ | ||
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\mathbf a \cdot \mathbf b = a \, b \: \cos(\theta_a -\theta_b) | \mathbf a \cdot \mathbf b = a \, b \: \cos(\theta_a -\theta_b) | ||
\end{align*} | \end{align*} | ||
- | **Hint: ** Work backwards, expressing $\cos(\theta_a -\theta_b)$ in terms of $\cos\theta_a$, | + | ++ Hint: | $\quad$ |
b) As a shortcut to the explicit calculation of a) one can introduce the coordinates $a_1 = a \, \cos\theta_a$ and $a_2 = a \, \sin\theta_a$, | b) As a shortcut to the explicit calculation of a) one can introduce the coordinates $a_1 = a \, \cos\theta_a$ and $a_2 = a \, \sin\theta_a$, | ||
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\mathbf b = \begin{pmatrix} b_1 \\ b_2 \end{pmatrix} | \mathbf b = \begin{pmatrix} b_1 \\ b_2 \end{pmatrix} | ||
\] | \] | ||
- | How does the product $\mathbf a \cdot \mathbf b$ look like in terms of these coordinates? | + | How does the product $\mathbf a \cdot \mathbf b$ look like in terms of these coordinates? |
- | c) How do the arguments in a) and b) change for $D$ dimensional vectors that are represented as linear combinations of a set of orthonormal basis vectors $\hat{\boldsymbol e}_1, \dots, \hat{\boldsymbol e}_D$?\\ | + | c) How do the arguments in a) and b) change for $D$ dimensional vectors that are represented as linear combinations of a set of orthonormal basis vectors $\hat{\boldsymbol e}_1, \dots, \hat{\boldsymbol e}_D$? |
- | :!: What changes when the basis is not orthonormal? | + | :!: What changes when the basis is not orthonormal? |
<wrap # | <wrap # | ||
** Scalar product on $\mathbb{R}^D$** \\ | ** Scalar product on $\mathbb{R}^D$** \\ | ||
- | Show that the scalar product on $\mathbb{R}^D$ takes exactly the same form as for the complex case, [[# | + | Show that the scalar product on $\mathbb{R}^D$ takes exactly the same form as for the complex case, [[# |
<wrap # | <wrap # | ||
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a_{ij} \in \mathbb{C} | a_{ij} \in \mathbb{C} | ||
\end{align*} | \end{align*} | ||
- | Show to that end:\\ | + | Show to that end: |
a) The matrices $\sigma_0$, $\dots$, $\sigma_4$ are linearly independent.\\ | a) The matrices $\sigma_0$, $\dots$, $\sigma_4$ are linearly independent.\\ | ||
b) $\displaystyle x_0, \dots, x_4 \in \mathbb{R} | b) $\displaystyle x_0, \dots, x_4 \in \mathbb{R} | ||
c) $\displaystyle M \in \mathbb{H} | c) $\displaystyle M \in \mathbb{H} | ||
- | :!: What about linear combinations with coefficients $z_1, \dots, | + | :!: What about linear combinations with coefficients $z_0, \dots, |
~~DISCUSSION|Questions, | ~~DISCUSSION|Questions, | ||
+ |
book/chap2/2.8_cartesian_coordinates.1636214488.txt.gz · Last modified: 2021/11/06 17:01 by abril