What is the Euclidean inner product intuition? [duplicate]

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  • What does the dot product of two vectors represent?

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The Euclidean inner product $<x,y>$ of the vectors $x , y in mathbbR^n$ is defined by:



$langle x,yrangle = x_1y_1 + x_2y_2 + x_3y_3 + ... + x_ny_n$



I am unable to find the intuition behind this? Why do we need this inner product? What happens to the vectors under equation and what does the scalar answer tell us?



P.S. I have already seareched it, most the articles take it into geometric terms and introduce $costheta$. Can anybody help me visualize thing without angular stuff?



Edit: Question addressed here uses the angle to explain geometric dot product. I am wondering if there exist some explanation for dot product in Vector Space.







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marked as duplicate by Lee Mosher, Travis, JavaMan, Parcly Taxel, user223391 Jul 29 at 22:01


This question has been asked before and already has an answer. If those answers do not fully address your question, please ask a new question.










  • 2




    Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
    – Suzet
    Jul 24 at 1:24







  • 1




    Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
    – JavaMan
    Jul 24 at 2:07











  • I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
    – David K
    Jul 24 at 2:14














up vote
5
down vote

favorite
1













This question already has an answer here:



  • What does the dot product of two vectors represent?

    7 answers



The Euclidean inner product $<x,y>$ of the vectors $x , y in mathbbR^n$ is defined by:



$langle x,yrangle = x_1y_1 + x_2y_2 + x_3y_3 + ... + x_ny_n$



I am unable to find the intuition behind this? Why do we need this inner product? What happens to the vectors under equation and what does the scalar answer tell us?



P.S. I have already seareched it, most the articles take it into geometric terms and introduce $costheta$. Can anybody help me visualize thing without angular stuff?



Edit: Question addressed here uses the angle to explain geometric dot product. I am wondering if there exist some explanation for dot product in Vector Space.







share|cite|improve this question













marked as duplicate by Lee Mosher, Travis, JavaMan, Parcly Taxel, user223391 Jul 29 at 22:01


This question has been asked before and already has an answer. If those answers do not fully address your question, please ask a new question.










  • 2




    Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
    – Suzet
    Jul 24 at 1:24







  • 1




    Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
    – JavaMan
    Jul 24 at 2:07











  • I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
    – David K
    Jul 24 at 2:14












up vote
5
down vote

favorite
1









up vote
5
down vote

favorite
1






1






This question already has an answer here:



  • What does the dot product of two vectors represent?

    7 answers



The Euclidean inner product $<x,y>$ of the vectors $x , y in mathbbR^n$ is defined by:



$langle x,yrangle = x_1y_1 + x_2y_2 + x_3y_3 + ... + x_ny_n$



I am unable to find the intuition behind this? Why do we need this inner product? What happens to the vectors under equation and what does the scalar answer tell us?



P.S. I have already seareched it, most the articles take it into geometric terms and introduce $costheta$. Can anybody help me visualize thing without angular stuff?



Edit: Question addressed here uses the angle to explain geometric dot product. I am wondering if there exist some explanation for dot product in Vector Space.







share|cite|improve this question














This question already has an answer here:



  • What does the dot product of two vectors represent?

    7 answers



The Euclidean inner product $<x,y>$ of the vectors $x , y in mathbbR^n$ is defined by:



$langle x,yrangle = x_1y_1 + x_2y_2 + x_3y_3 + ... + x_ny_n$



I am unable to find the intuition behind this? Why do we need this inner product? What happens to the vectors under equation and what does the scalar answer tell us?



P.S. I have already seareched it, most the articles take it into geometric terms and introduce $costheta$. Can anybody help me visualize thing without angular stuff?



Edit: Question addressed here uses the angle to explain geometric dot product. I am wondering if there exist some explanation for dot product in Vector Space.





This question already has an answer here:



  • What does the dot product of two vectors represent?

    7 answers









share|cite|improve this question












share|cite|improve this question




share|cite|improve this question








edited Jul 24 at 2:50









max_zorn

3,15151028




3,15151028









asked Jul 24 at 1:22









Wasiq Noor

634




634




marked as duplicate by Lee Mosher, Travis, JavaMan, Parcly Taxel, user223391 Jul 29 at 22:01


This question has been asked before and already has an answer. If those answers do not fully address your question, please ask a new question.






marked as duplicate by Lee Mosher, Travis, JavaMan, Parcly Taxel, user223391 Jul 29 at 22:01


This question has been asked before and already has an answer. If those answers do not fully address your question, please ask a new question.









  • 2




    Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
    – Suzet
    Jul 24 at 1:24







  • 1




    Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
    – JavaMan
    Jul 24 at 2:07











  • I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
    – David K
    Jul 24 at 2:14












  • 2




    Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
    – Suzet
    Jul 24 at 1:24







  • 1




    Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
    – JavaMan
    Jul 24 at 2:07











  • I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
    – David K
    Jul 24 at 2:14







2




2




Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
– Suzet
Jul 24 at 1:24





Well, the intuition one must have of the inner product precisely is this "angular stuff", to my opinion.
– Suzet
Jul 24 at 1:24





1




1




Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
– JavaMan
Jul 24 at 2:07





Small $LaTeX$ note: "langle" and "rangle" look nicer than the greater than/less than symbol: They typeset as $langle -, - rangle$.
– JavaMan
Jul 24 at 2:07













I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
– David K
Jul 24 at 2:14




I'm answering this here rather than calling it a duplicate because it explicitly asks for explanations that are not "angular." I think @LeeMosher's answer to the other question actually is such an answer but the others mostly are not.
– David K
Jul 24 at 2:14










3 Answers
3






active

oldest

votes

















up vote
1
down vote













You are probably familiar with the following formula involving
a vector $x = (x_1, ldots, x_n) in mathbb R^n$
and $n$ constants $a_1, ldots, a_n$ that are not all zero:
$$
a_1 x_1 + a_2 x_2 + cdots + a_n x_n = 0.
$$



This formula describes an $(n-1)$-dimensional hyperplane in $mathbb R^n.$
Let's call that hyperplane $A.$ That is, any vector $x$ that satisfies the formula lies in the hyperplane $A.$



If we define a vector $a = (a_1, ldots, a_n),$
then another way to write the formula is
$$ langle x, arangle = 0. $$



Now if we choose an arbitrary vector $x in mathbb R^n,$
it may happen that $langle x, arangle neq 0.$
If we have two such vectors, let's say $x'$ and $x'',$
such that $langle x', arangle > 0$ and $langle x'', arangle > 0,$
then $x'$ and $x''$ will be on the same side of the hyperplane $A.$
But if $langle x', arangle < 0 < langle x'', arangle$ then the vectors are on opposite sides.



For a given vector $x,$ suppose you find a vector $y$ such that
$x - langle x, arangle y$ is in the hyperplane $A.$
Then $x' - langle x', arangle y$ also is in the hyperplane $A$
for any other vector $x'.$
That is, $langle x, arangle$ tells you how many times the length of $y$
you have to travel in the direction of $y$ to get from $x$ to the hyperplane,
or in other words, $langle x', arangle$ is a kind of measurement of the distance of $x$ from the hyperplane (measured in some particular units in some particular direction).



All of this works without any "angles" (unless you consider "parallel" to be a "zero angle").



You don't even need
$(x_1, ldots, x_n)$ to be coordinates over an orthonormal basis,
although if the basis is orthonormal then other nice results follow.
For example,
$$sqrtlangle x, xrangle = sqrtx_1^2 + x_2^2 + cdots + x_n^2,$$
which is the length of $x$ (according to the Pythagorean Theorem)
if the basis of $(x_1, ldots, x_n)$ is orthonormal.
Admittedly, to speak of "normals" one must have a concept of things being perpendicular, which starts to sound like we're dealing with angles again.
But they're right angles, which are especially simple to work with.






share|cite|improve this answer




























    up vote
    0
    down vote













    $<x,y>$ is positive if and only if the angle between $x$ and $y$ is less than 90 degrees. $<x,y>$ is sort of like a measure of how pointed in the same direction $x$ and $y$ are.



    The geometry of least squares problems and separating hyperplanes is useful for gaining intuition about inner products.






    share|cite|improve this answer




























      up vote
      0
      down vote













      The intuition is gathered from the following, given by the Law of Cosines



      $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$enter image description here



      $$ | a-b|^2 = (a-b)^2cdot(a-b)^2 $$
      $$ | a-b|^2 = acdot a - acdot b - bcdot a + b cdot b $$



      useful to note that $a cdot a = | a| $



      $$ | a-b|^2 = |a | - acdot b - bcdot a + | b|$$



      further more we have $ a cdot b = bcdot a $
      $$ | a-b|^2 = |a | - 2 acdot b + | b|$$



      so we have



      $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$



      $$ | a|^2 - 2 a cdot b + | b|^2 = |a|^2 + |b|^2 - 2|a| |b| cos(theta) - 2 a cdot b = -2 |a | |b| cos(theta) $$



      yielding finally
      $$a cdot b = | a | | b| cos(theta) $$



      Now suppose that



      $$ |a| = |b| =1 $$
      $$ a cdot b = 1 cdot 1 cos(theta) = cos(theta)$$
      ok when is this negative. We have a unit circle here for vectors



      $$ a cdot b = cos( theta) < 0 implies fracnpi2 < theta < frac3npi2 $$



      that is we are in one part of the circle. However, it goes on forever.



      Note from lamar






      share|cite|improve this answer




























        3 Answers
        3






        active

        oldest

        votes








        3 Answers
        3






        active

        oldest

        votes









        active

        oldest

        votes






        active

        oldest

        votes








        up vote
        1
        down vote













        You are probably familiar with the following formula involving
        a vector $x = (x_1, ldots, x_n) in mathbb R^n$
        and $n$ constants $a_1, ldots, a_n$ that are not all zero:
        $$
        a_1 x_1 + a_2 x_2 + cdots + a_n x_n = 0.
        $$



        This formula describes an $(n-1)$-dimensional hyperplane in $mathbb R^n.$
        Let's call that hyperplane $A.$ That is, any vector $x$ that satisfies the formula lies in the hyperplane $A.$



        If we define a vector $a = (a_1, ldots, a_n),$
        then another way to write the formula is
        $$ langle x, arangle = 0. $$



        Now if we choose an arbitrary vector $x in mathbb R^n,$
        it may happen that $langle x, arangle neq 0.$
        If we have two such vectors, let's say $x'$ and $x'',$
        such that $langle x', arangle > 0$ and $langle x'', arangle > 0,$
        then $x'$ and $x''$ will be on the same side of the hyperplane $A.$
        But if $langle x', arangle < 0 < langle x'', arangle$ then the vectors are on opposite sides.



        For a given vector $x,$ suppose you find a vector $y$ such that
        $x - langle x, arangle y$ is in the hyperplane $A.$
        Then $x' - langle x', arangle y$ also is in the hyperplane $A$
        for any other vector $x'.$
        That is, $langle x, arangle$ tells you how many times the length of $y$
        you have to travel in the direction of $y$ to get from $x$ to the hyperplane,
        or in other words, $langle x', arangle$ is a kind of measurement of the distance of $x$ from the hyperplane (measured in some particular units in some particular direction).



        All of this works without any "angles" (unless you consider "parallel" to be a "zero angle").



        You don't even need
        $(x_1, ldots, x_n)$ to be coordinates over an orthonormal basis,
        although if the basis is orthonormal then other nice results follow.
        For example,
        $$sqrtlangle x, xrangle = sqrtx_1^2 + x_2^2 + cdots + x_n^2,$$
        which is the length of $x$ (according to the Pythagorean Theorem)
        if the basis of $(x_1, ldots, x_n)$ is orthonormal.
        Admittedly, to speak of "normals" one must have a concept of things being perpendicular, which starts to sound like we're dealing with angles again.
        But they're right angles, which are especially simple to work with.






        share|cite|improve this answer

























          up vote
          1
          down vote













          You are probably familiar with the following formula involving
          a vector $x = (x_1, ldots, x_n) in mathbb R^n$
          and $n$ constants $a_1, ldots, a_n$ that are not all zero:
          $$
          a_1 x_1 + a_2 x_2 + cdots + a_n x_n = 0.
          $$



          This formula describes an $(n-1)$-dimensional hyperplane in $mathbb R^n.$
          Let's call that hyperplane $A.$ That is, any vector $x$ that satisfies the formula lies in the hyperplane $A.$



          If we define a vector $a = (a_1, ldots, a_n),$
          then another way to write the formula is
          $$ langle x, arangle = 0. $$



          Now if we choose an arbitrary vector $x in mathbb R^n,$
          it may happen that $langle x, arangle neq 0.$
          If we have two such vectors, let's say $x'$ and $x'',$
          such that $langle x', arangle > 0$ and $langle x'', arangle > 0,$
          then $x'$ and $x''$ will be on the same side of the hyperplane $A.$
          But if $langle x', arangle < 0 < langle x'', arangle$ then the vectors are on opposite sides.



          For a given vector $x,$ suppose you find a vector $y$ such that
          $x - langle x, arangle y$ is in the hyperplane $A.$
          Then $x' - langle x', arangle y$ also is in the hyperplane $A$
          for any other vector $x'.$
          That is, $langle x, arangle$ tells you how many times the length of $y$
          you have to travel in the direction of $y$ to get from $x$ to the hyperplane,
          or in other words, $langle x', arangle$ is a kind of measurement of the distance of $x$ from the hyperplane (measured in some particular units in some particular direction).



          All of this works without any "angles" (unless you consider "parallel" to be a "zero angle").



          You don't even need
          $(x_1, ldots, x_n)$ to be coordinates over an orthonormal basis,
          although if the basis is orthonormal then other nice results follow.
          For example,
          $$sqrtlangle x, xrangle = sqrtx_1^2 + x_2^2 + cdots + x_n^2,$$
          which is the length of $x$ (according to the Pythagorean Theorem)
          if the basis of $(x_1, ldots, x_n)$ is orthonormal.
          Admittedly, to speak of "normals" one must have a concept of things being perpendicular, which starts to sound like we're dealing with angles again.
          But they're right angles, which are especially simple to work with.






          share|cite|improve this answer























            up vote
            1
            down vote










            up vote
            1
            down vote









            You are probably familiar with the following formula involving
            a vector $x = (x_1, ldots, x_n) in mathbb R^n$
            and $n$ constants $a_1, ldots, a_n$ that are not all zero:
            $$
            a_1 x_1 + a_2 x_2 + cdots + a_n x_n = 0.
            $$



            This formula describes an $(n-1)$-dimensional hyperplane in $mathbb R^n.$
            Let's call that hyperplane $A.$ That is, any vector $x$ that satisfies the formula lies in the hyperplane $A.$



            If we define a vector $a = (a_1, ldots, a_n),$
            then another way to write the formula is
            $$ langle x, arangle = 0. $$



            Now if we choose an arbitrary vector $x in mathbb R^n,$
            it may happen that $langle x, arangle neq 0.$
            If we have two such vectors, let's say $x'$ and $x'',$
            such that $langle x', arangle > 0$ and $langle x'', arangle > 0,$
            then $x'$ and $x''$ will be on the same side of the hyperplane $A.$
            But if $langle x', arangle < 0 < langle x'', arangle$ then the vectors are on opposite sides.



            For a given vector $x,$ suppose you find a vector $y$ such that
            $x - langle x, arangle y$ is in the hyperplane $A.$
            Then $x' - langle x', arangle y$ also is in the hyperplane $A$
            for any other vector $x'.$
            That is, $langle x, arangle$ tells you how many times the length of $y$
            you have to travel in the direction of $y$ to get from $x$ to the hyperplane,
            or in other words, $langle x', arangle$ is a kind of measurement of the distance of $x$ from the hyperplane (measured in some particular units in some particular direction).



            All of this works without any "angles" (unless you consider "parallel" to be a "zero angle").



            You don't even need
            $(x_1, ldots, x_n)$ to be coordinates over an orthonormal basis,
            although if the basis is orthonormal then other nice results follow.
            For example,
            $$sqrtlangle x, xrangle = sqrtx_1^2 + x_2^2 + cdots + x_n^2,$$
            which is the length of $x$ (according to the Pythagorean Theorem)
            if the basis of $(x_1, ldots, x_n)$ is orthonormal.
            Admittedly, to speak of "normals" one must have a concept of things being perpendicular, which starts to sound like we're dealing with angles again.
            But they're right angles, which are especially simple to work with.






            share|cite|improve this answer













            You are probably familiar with the following formula involving
            a vector $x = (x_1, ldots, x_n) in mathbb R^n$
            and $n$ constants $a_1, ldots, a_n$ that are not all zero:
            $$
            a_1 x_1 + a_2 x_2 + cdots + a_n x_n = 0.
            $$



            This formula describes an $(n-1)$-dimensional hyperplane in $mathbb R^n.$
            Let's call that hyperplane $A.$ That is, any vector $x$ that satisfies the formula lies in the hyperplane $A.$



            If we define a vector $a = (a_1, ldots, a_n),$
            then another way to write the formula is
            $$ langle x, arangle = 0. $$



            Now if we choose an arbitrary vector $x in mathbb R^n,$
            it may happen that $langle x, arangle neq 0.$
            If we have two such vectors, let's say $x'$ and $x'',$
            such that $langle x', arangle > 0$ and $langle x'', arangle > 0,$
            then $x'$ and $x''$ will be on the same side of the hyperplane $A.$
            But if $langle x', arangle < 0 < langle x'', arangle$ then the vectors are on opposite sides.



            For a given vector $x,$ suppose you find a vector $y$ such that
            $x - langle x, arangle y$ is in the hyperplane $A.$
            Then $x' - langle x', arangle y$ also is in the hyperplane $A$
            for any other vector $x'.$
            That is, $langle x, arangle$ tells you how many times the length of $y$
            you have to travel in the direction of $y$ to get from $x$ to the hyperplane,
            or in other words, $langle x', arangle$ is a kind of measurement of the distance of $x$ from the hyperplane (measured in some particular units in some particular direction).



            All of this works without any "angles" (unless you consider "parallel" to be a "zero angle").



            You don't even need
            $(x_1, ldots, x_n)$ to be coordinates over an orthonormal basis,
            although if the basis is orthonormal then other nice results follow.
            For example,
            $$sqrtlangle x, xrangle = sqrtx_1^2 + x_2^2 + cdots + x_n^2,$$
            which is the length of $x$ (according to the Pythagorean Theorem)
            if the basis of $(x_1, ldots, x_n)$ is orthonormal.
            Admittedly, to speak of "normals" one must have a concept of things being perpendicular, which starts to sound like we're dealing with angles again.
            But they're right angles, which are especially simple to work with.







            share|cite|improve this answer













            share|cite|improve this answer



            share|cite|improve this answer











            answered Jul 24 at 2:09









            David K

            48.2k340107




            48.2k340107




















                up vote
                0
                down vote













                $<x,y>$ is positive if and only if the angle between $x$ and $y$ is less than 90 degrees. $<x,y>$ is sort of like a measure of how pointed in the same direction $x$ and $y$ are.



                The geometry of least squares problems and separating hyperplanes is useful for gaining intuition about inner products.






                share|cite|improve this answer

























                  up vote
                  0
                  down vote













                  $<x,y>$ is positive if and only if the angle between $x$ and $y$ is less than 90 degrees. $<x,y>$ is sort of like a measure of how pointed in the same direction $x$ and $y$ are.



                  The geometry of least squares problems and separating hyperplanes is useful for gaining intuition about inner products.






                  share|cite|improve this answer























                    up vote
                    0
                    down vote










                    up vote
                    0
                    down vote









                    $<x,y>$ is positive if and only if the angle between $x$ and $y$ is less than 90 degrees. $<x,y>$ is sort of like a measure of how pointed in the same direction $x$ and $y$ are.



                    The geometry of least squares problems and separating hyperplanes is useful for gaining intuition about inner products.






                    share|cite|improve this answer













                    $<x,y>$ is positive if and only if the angle between $x$ and $y$ is less than 90 degrees. $<x,y>$ is sort of like a measure of how pointed in the same direction $x$ and $y$ are.



                    The geometry of least squares problems and separating hyperplanes is useful for gaining intuition about inner products.







                    share|cite|improve this answer













                    share|cite|improve this answer



                    share|cite|improve this answer











                    answered Jul 24 at 1:29









                    ted

                    446312




                    446312




















                        up vote
                        0
                        down vote













                        The intuition is gathered from the following, given by the Law of Cosines



                        $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$enter image description here



                        $$ | a-b|^2 = (a-b)^2cdot(a-b)^2 $$
                        $$ | a-b|^2 = acdot a - acdot b - bcdot a + b cdot b $$



                        useful to note that $a cdot a = | a| $



                        $$ | a-b|^2 = |a | - acdot b - bcdot a + | b|$$



                        further more we have $ a cdot b = bcdot a $
                        $$ | a-b|^2 = |a | - 2 acdot b + | b|$$



                        so we have



                        $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$



                        $$ | a|^2 - 2 a cdot b + | b|^2 = |a|^2 + |b|^2 - 2|a| |b| cos(theta) - 2 a cdot b = -2 |a | |b| cos(theta) $$



                        yielding finally
                        $$a cdot b = | a | | b| cos(theta) $$



                        Now suppose that



                        $$ |a| = |b| =1 $$
                        $$ a cdot b = 1 cdot 1 cos(theta) = cos(theta)$$
                        ok when is this negative. We have a unit circle here for vectors



                        $$ a cdot b = cos( theta) < 0 implies fracnpi2 < theta < frac3npi2 $$



                        that is we are in one part of the circle. However, it goes on forever.



                        Note from lamar






                        share|cite|improve this answer

























                          up vote
                          0
                          down vote













                          The intuition is gathered from the following, given by the Law of Cosines



                          $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$enter image description here



                          $$ | a-b|^2 = (a-b)^2cdot(a-b)^2 $$
                          $$ | a-b|^2 = acdot a - acdot b - bcdot a + b cdot b $$



                          useful to note that $a cdot a = | a| $



                          $$ | a-b|^2 = |a | - acdot b - bcdot a + | b|$$



                          further more we have $ a cdot b = bcdot a $
                          $$ | a-b|^2 = |a | - 2 acdot b + | b|$$



                          so we have



                          $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$



                          $$ | a|^2 - 2 a cdot b + | b|^2 = |a|^2 + |b|^2 - 2|a| |b| cos(theta) - 2 a cdot b = -2 |a | |b| cos(theta) $$



                          yielding finally
                          $$a cdot b = | a | | b| cos(theta) $$



                          Now suppose that



                          $$ |a| = |b| =1 $$
                          $$ a cdot b = 1 cdot 1 cos(theta) = cos(theta)$$
                          ok when is this negative. We have a unit circle here for vectors



                          $$ a cdot b = cos( theta) < 0 implies fracnpi2 < theta < frac3npi2 $$



                          that is we are in one part of the circle. However, it goes on forever.



                          Note from lamar






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                            The intuition is gathered from the following, given by the Law of Cosines



                            $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$enter image description here



                            $$ | a-b|^2 = (a-b)^2cdot(a-b)^2 $$
                            $$ | a-b|^2 = acdot a - acdot b - bcdot a + b cdot b $$



                            useful to note that $a cdot a = | a| $



                            $$ | a-b|^2 = |a | - acdot b - bcdot a + | b|$$



                            further more we have $ a cdot b = bcdot a $
                            $$ | a-b|^2 = |a | - 2 acdot b + | b|$$



                            so we have



                            $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$



                            $$ | a|^2 - 2 a cdot b + | b|^2 = |a|^2 + |b|^2 - 2|a| |b| cos(theta) - 2 a cdot b = -2 |a | |b| cos(theta) $$



                            yielding finally
                            $$a cdot b = | a | | b| cos(theta) $$



                            Now suppose that



                            $$ |a| = |b| =1 $$
                            $$ a cdot b = 1 cdot 1 cos(theta) = cos(theta)$$
                            ok when is this negative. We have a unit circle here for vectors



                            $$ a cdot b = cos( theta) < 0 implies fracnpi2 < theta < frac3npi2 $$



                            that is we are in one part of the circle. However, it goes on forever.



                            Note from lamar






                            share|cite|improve this answer













                            The intuition is gathered from the following, given by the Law of Cosines



                            $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$enter image description here



                            $$ | a-b|^2 = (a-b)^2cdot(a-b)^2 $$
                            $$ | a-b|^2 = acdot a - acdot b - bcdot a + b cdot b $$



                            useful to note that $a cdot a = | a| $



                            $$ | a-b|^2 = |a | - acdot b - bcdot a + | b|$$



                            further more we have $ a cdot b = bcdot a $
                            $$ | a-b|^2 = |a | - 2 acdot b + | b|$$



                            so we have



                            $$| a -b|^2 = | a|^2 + | b|^2 - 2| a|^2 | b|^2cos(theta) $$



                            $$ | a|^2 - 2 a cdot b + | b|^2 = |a|^2 + |b|^2 - 2|a| |b| cos(theta) - 2 a cdot b = -2 |a | |b| cos(theta) $$



                            yielding finally
                            $$a cdot b = | a | | b| cos(theta) $$



                            Now suppose that



                            $$ |a| = |b| =1 $$
                            $$ a cdot b = 1 cdot 1 cos(theta) = cos(theta)$$
                            ok when is this negative. We have a unit circle here for vectors



                            $$ a cdot b = cos( theta) < 0 implies fracnpi2 < theta < frac3npi2 $$



                            that is we are in one part of the circle. However, it goes on forever.



                            Note from lamar







                            share|cite|improve this answer













                            share|cite|improve this answer



                            share|cite|improve this answer











                            answered Jul 24 at 2:17









                            RHowe

                            1,010815




                            1,010815












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