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In [[mathematics]], one can often define a '''direct product''' of objects
[[File:Doppler effect diagrammatic.svg|thumb|250px|Change of wavelength caused by motion of the source]]
already known, giving a new one. This generalizes the [[Cartesian product]] of the underlying sets, together with a suitably defined structure on the product set.
[[File:Dopplerfrequenz.gif|thumb|250px|An animation illustrating how the Doppler effect causes a car engine or siren to sound higher in pitch when it is approaching than when it is receding. The pink circles represent sound waves. ]]
More abstractly, one talks about the [[Product (category theory)|product in category theory]], which formalizes these notions.
[[File:Doppler hattyu.jpg|thumb|220px|Doppler effect of water flow around a swan]]


The '''Doppler effect''' (or '''Doppler shift''') is the change in [[frequency]] of a [[wave]] (or other periodic event) for an [[observer (physics)|observer]] moving relative to its source. It is named after the [[Austria]]n physicist [[Christian Doppler]], who proposed it in 1842 in [[Prague]]. It is commonly heard when a vehicle sounding a [[siren (noisemaker)|siren]] or horn approaches, passes, and recedes from an observer. Compared to the emitted frequency, the received frequency is higher during the approach, identical at the instant of passing by, and lower during the recession.
Examples are the product of sets (see [[Cartesian product]]), groups (described below), the [[product of rings]] and of other [[abstract algebra|algebraic structures]]. The [[product topology|product of topological spaces]] is another instance.


When the source of the waves is moving toward the observer, each successive wave [[Crest (physics)|crest]] is emitted from a position closer to the observer than the previous wave. Therefore, each wave takes slightly less time to reach the observer than the previous wave. Hence, the time between the arrival of successive wave crests at the observer is reduced, causing an increase in the frequency. While they are travelling, the distance between successive wave fronts is reduced, so the waves "bunch together".  Conversely, if the source of waves is moving away from the observer, each wave is emitted from a position farther from the observer than the previous wave, so the arrival time between successive waves is increased, reducing the frequency. The distance between successive wave fronts is then increased, so the waves "spread out".
There is also the [[direct sum]] – in some areas this is used interchangeably, in others it is a different concept.


For waves that propagate in a medium, such as [[sound]] waves, the velocity of the observer and of the source are relative to the medium in which the waves are transmitted. The total Doppler effect may therefore result from motion of the source, motion of the observer, or motion of the medium. Each of these effects is analyzed separately. For waves which do not require a medium, such as light or [[gravity]] in [[general relativity]], only the relative difference in velocity between the observer and the source needs to be considered.
== Examples ==


==Development==
* If we think of <math>\mathbb{R}</math> as the [[set (mathematics)|set]] of real numbers, then the direct product <math>\mathbb{R}\times \mathbb{R}</math> is precisely just the [[cartesian product]], <math>\{ (x,y) | x,y \in \mathbb{R} \}</math>.
Doppler first proposed this effect in 1842 in his treatise "''[[Über das farbige Licht der Doppelsterne und einiger anderer Gestirne des Himmels]]''" (On the coloured light of the [[binary stars]] and some other stars of the heavens).<ref name="AlecEden">Alec Eden ''The search for Christian Doppler'',Springer-Verlag, Wien 1992. Contains a facsimile edition with an [[English language|English]] translation.</ref> The hypothesis was tested for sound waves by [[C. H. D. Buys Ballot|Buys Ballot]] in 1845.<ref>{{cite journal | last=Buys Ballot | title=Akustische Versuche auf der Niederländischen Eisenbahn, nebst gelegentlichen Bemerkungen zur Theorie des Hrn. Prof. Doppler (in German) | journal=Annalen der Physik und Chemie | date=1845 | volume=11 | pages=321–351 | doi=10.1002/andp.18451421102}}</ref>
He confirmed that the sound's [[Pitch (music)#Pitch and frequency|pitch]] was higher than the emitted frequency when the sound source approached him, and lower than the emitted frequency when the sound source receded from him. [[Hippolyte Fizeau]] discovered independently the same phenomenon on [[electromagnetic wave]]s in 1848 (in France, the effect is sometimes called "effet Doppler-Fizeau" but that name was not adopted by the rest of the world as Fizeau's discovery was six years after Doppler's proposal).<ref>Fizeau: "Acoustique et optique". ''Lecture, [[Philomatic Society|Société Philomathique]] de Paris'', 29 December 1848. According to Becker(pg. 109), this was never published, but recounted by M. Moigno(1850): "Répertoire d'optique moderne" (in French), vol 3. pp 1165-1203 and later in full by Fizeau, "Des effets du mouvement sur le ton des vibrations sonores et sur la longeur d'onde des rayons de lumière"; [Paris, 1870]. ''Annales de Chimie et de Physique'', 19, 211-221.
* Becker (2011). Barbara J. Becker, ''Unravelling Starlight: William and Margaret Huggins and the Rise of the New Astronomy'', illustrated Edition, [[Cambridge University Press]], 2011; ISBN 110700229X, 9781107002296.</ref> In Britain, [[John Scott Russell]] made an experimental study of the Doppler effect (1848).<ref>{{cite journal | last=Scott Russell | first=John | url=http://www.ma.hw.ac.uk/~chris/doppler.html | title=On certain effects produced on sound by the rapid motion of the observer | journal=Report of the Eighteenth Meeting of the British Association for the Advancement of Science | date=1848 | volume=18 | issue=7 | pages=37–38 | publisher=John Murray, London in 1849 | accessdate=2008-07-08 }}</ref>


==General==
* If we think of <math>\mathbb{R}</math> as the [[group (mathematics)|group]] of real numbers under addition, then the direct product <math>\mathbb{R}\times \mathbb{R}</math> still consists of <math>\{ (x,y) | x,y \in \mathbb{R} \}</math>. The difference between this and the preceding example is that <math>\mathbb{R}\times \mathbb{R}</math> is now a group.  We have to also say how to add their elements. This is done by letting <math>(a,b) + (c,d) = (a+c, b+d)</math>.


In classical physics, where the speeds of source and the receiver relative to the medium are lower than the velocity of waves in the medium, the relationship between observed frequency <math>f</math> and emitted frequency <math>f_\text{0}</math> is given by:<ref name=encphysci>{{cite book
* If we think of <math>\mathbb{R}</math> as the [[ring (mathematics)|ring]] of real numbers, then the direct product <math>\mathbb{R}\times \mathbb{R}</math> again consists of <math>\{ (x,y) | x,y \in \mathbb{R} \}</math>.  To make this a ring, we say how their elements are added, <math>(a,b) + (c,d) = (a+c, b+d)</math>, and how they are multiplied <math>(a,b) (c,d) = (ac, bd)</math>.
|title=Encyclopedia of Physical Science
|first1=Joe
|last1=Rosen
|first2=Lisa Quinn
|last2=Gothard
|publisher=Infobase Publishing
|date=2009
|isbn=0-8160-7011-3
|page=155
|url=http://books.google.com/books?id=avyQ64LIJa0C}}, [http://books.google.com/books?id=avyQ64LIJa0C&pg=PA155 Extract of page 155]</ref>
::<math>f = \left( \frac{c + v_\text{r}}{c + v_\text{s}} \right) f_0 \,</math>
:where
::<math>c \;</math> is the velocity of waves in the medium;
::<math>v_\text{r} \,</math> is the velocity of the receiver relative to the medium; positive if the receiver is moving towards the source (and negative in the other direction);
::<math>v_\text{s} \,</math> is the velocity of the source relative to the medium; positive if the source is moving away from the receiver (and negative in the other direction).


The frequency is decreased if either is moving away from the other.
* However, if we think of <math>\mathbb{R}</math> as the [[field (mathematics)|field]] of real numbers, then the direct product <math>\mathbb{R}\times \mathbb{R}</math> does not exist – naively defining <math>\{ (x,y) | x,y \in \mathbb{R} \}</math> in a similar manner to the above examples would not result in a field since the element <math>(1,0)</math> does not have a multiplicative inverse.


The above formula assumes that the source is either directly approaching or receding from the observer. If the source approaches the observer at an angle (but still with a constant velocity), the observed frequency that is first heard is higher than the object's emitted frequency. Thereafter, there is a [[monotonic]] decrease in the observed frequency as it gets closer to the observer, through equality when it is coming from a direction perpendicular to the relative motion (and was emitted at the point of closest approach; but when the wave is received, the source and observer will no longer be at their closest), and a continued monotonic decrease as it recedes from the observer. When the observer is very close to the path of the object, the transition from high to low frequency is very abrupt. When the observer is far from the path of the object, the transition from high to low frequency is gradual.
In a similar manner, we can talk about the product of more than two objects, e.g. <math>\mathbb{R} \times \mathbb{R} \times \mathbb{R} \times \mathbb{R}</math>. We can even talk about product of infinitely many objects, e.g. <math>\mathbb{R} \times \mathbb{R} \times \mathbb{R} \times \dotsb</math>.


If the speeds <math>v_\text{s} \,</math> and <math>v_\text{r} \,</math> are small compared to the speed of the wave, the relationship between observed frequency <math>f</math> and emitted frequency <math>f_\text{0}</math> is approximately<ref name=encphysci />
== Group direct product ==
{|
{{main|Direct product of groups}}
|-
In [[group (mathematics)|group theory]] one can define the direct product of two
!Observed frequency||Change in frequency
groups (''G'', *) and (''H'', ●), denoted by ''G'' &times; ''H''. For [[abelian group]]s which are written additively, it may also be called the [[Direct sum of groups|direct sum of two groups]], denoted by <math>G \oplus H</math>.
|-
|width=70%|<center><math>f=\left(1+\frac{\Delta v}{c}\right)f_0</math></center>|||<center><math>\Delta f=\frac{\Delta v}{c}f_0</math></center>
|}


:where
It is defined as follows:
::<math>\Delta f = f - f_0 \,</math>
* the [[Set (mathematics)|set]] of the elements of the new group is the ''[[cartesian product]]'' of the sets of elements of ''G'' and ''H'', that is {(''g'', ''h''): ''g'' in ''G'', ''h'' in ''H''};
::<math>\Delta v = v_\text{r} - v_\text{s} \,</math> is the velocity of the receiver relative to the source: it is positive when the source and the receiver are moving towards each other.
* on these elements put an operation, defined elementwise: <center>(''g'', ''h'') &times; (''g' '', ''h' '') = (''g'' * ''g' '', ''h'' ● ''h' '')</center>
(Note the operation * may be the same as ●.)


{{hidden begin|title=Proof|toggle=left}}
This construction gives a new group. It has a [[normal subgroup]]
Given <math>f = \left( \frac{c + v_\text{r}}{c + v_\text{s}} \right) f_0 \,</math>
[[isomorphic]] to ''G'' (given by the elements of the form (''g'', 1)),
and one isomorphic to ''H'' (comprising the elements (1, ''h'')).


we divide for <math>c</math>
The reverse also holds, there is the following recognition theorem: If a group ''K'' contains two normal subgroups ''G'' and ''H'', such that ''K''= ''GH'' and the intersection of ''G'' and ''H'' contains only the identity, then ''K'' is isomorphic to ''G'' x ''H''. A relaxation of these conditions, requiring only one subgroup to be normal, gives the [[semidirect product]].


<math>f = \left( \frac{1 + \frac{v_\text{r}} {c}} {1 + \frac{v_\text{s}} {c}} \right) f_0  = \left( 1 + \frac{v_\text{r}}{c} \right) \left( \frac{1}{1 + \frac{v_\text{s}} {c}} \right) f_0 \,</math>
As an example, take as ''G'' and ''H'' two copies of the unique (up to
isomorphisms) group of order 2, ''C''<sub>2</sub>: say {1, ''a''} and {1, ''b''}. Then ''C''<sub>2</sub>&times;''C''<sub>2</sub> = {(1,1), (1,''b''), (''a'',1), (''a'',''b'')}, with the operation element by element. For instance, (1,''b'')*(''a'',1) = (1*''a'', ''b''*1) = (''a'',''b''), and (1,''b'')*(1,''b'') = (1,''b''<sup>2</sup>) = (1,1).


Since <math>\frac{v_\text{s}}{c} \ll 1</math> we can substitute the geometric expansion:
With a direct product, we get some natural [[group homomorphism]]s for free: the projection maps
:<math>\pi_1: G \times H \to G\quad \text{by} \quad \pi_1(g, h) = g</math>,
:<math>\pi_2: G \times H \to H\quad \text{by} \quad \pi_2(g, h) = h</math>
called the '''coordinate functions'''.


<math> \frac{1} {1 + \frac{v_\text{s}}{c}} \approx 1 - \frac{v_\text{s}}{c}</math>
Also, every homomorphism ''f'' to the direct product is totally determined by its component functions
{{hidden end}}
<math>f_i = \pi_i \circ f</math>.


{{gallery
For any group (''G'', *), and any integer ''n'' ≥ 0, multiple application of the direct product gives the group of all ''n''-[[tuple]]s  ''G''<sup>''n''</sup> (for ''n''&nbsp;=&nbsp;0 the trivial group). Examples:
|align=center
*'''Z'''<sup>''n''</sup>
|width=200
*'''R'''<sup>''n''</sup> (with additional [[vector space]] structure this is called [[Euclidean space]], see below)
|height=200
|lines=5


|File:Dopplereffectstationary.gif|alt1=|Stationary sound source produces sound waves at a constant frequency {{math|''f''}}, and the wave-fronts propagate symmetrically away from the source at a constant speed c. The distance between wave-fronts is the wavelength. All observers will hear the same frequency, which will be equal to the actual frequency of the source where {{math|''f'' {{=}} ''f''{{sub|0}} }}.
== Direct product of modules ==
The direct product for [[module (mathematics)|modules]] (not to be confused with the [[Tensor product of modules|tensor product]]) is very similar to the one defined for groups above, using the [[cartesian product]] with the operation of addition being componentwise, and the scalar multiplication just distributing over all the components. Starting from '''R''' we get [[Euclidean space]] '''R'''<sup>''n''</sup>, the prototypical example of a real ''n''-dimensional vector space. The direct product of '''R'''<sup>''m''</sup> and '''R'''<sup>''n''</sup> is '''R'''<sup>''m'' + ''n''</sup>.


|File:Dopplereffectsourcemovingrightatmach0.7.gif|alt2=|The same sound source is radiating sound waves at a constant frequency in the same medium. However, now the sound source is moving with a speed {{math|''υ''{{sub|s}} {{=}} 0.7 ''c''}} (Mach 0.7). Since the source is moving, the centre of each new wavefront is now slightly displaced to the right. As a result, the wave-fronts begin to bunch up on the right side (in front of) and spread further apart on the left side (behind) of the source. An observer in front of the source will hear a higher frequency
Note that a direct product for a finite index <math>\prod_{i=1}^n X_i </math> is identical to the [[Direct sum of modules|direct sum]] <math>\bigoplus_{i=1}^n X_i </math>. The direct sum and direct product differ only for infinite indices, where the elements of a direct sum are zero for all but for a finite number of entries. They are dual in the sense of [[category theory]]: the direct sum is the [[coproduct]], while the direct product is the product.
{{math|''f'' {{=}} {{sfrac|''c'' + 0|''c'' - 0.7''c''}} ''f''{{sub|0}} {{=}} 3.33 ''f''{{sub|0}} }}
and an observer behind the source will hear a lower frequency
{{math|''f'' {{=}} {{sfrac|''c'' - 0|''c'' + 0.7''c''}} ''f''{{sub|0}} {{=}} 0.59 ''f''{{sub|0}} }}.


|File:Dopplereffectsourcemovingrightatmach1.0.gif|alt3=|Now the source is moving at the speed of sound in the medium ({{math|''υ''{{sub|s}} {{=}} ''c''}}, or Mach 1). The wave fronts in front of the source are now all bunched up at the same point. As a result, an observer in front of the source will detect nothing until the source arrives where
For example, consider <math>X=\prod_{i=1}^\infty \mathbb{R} </math> and <math>Y=\bigoplus_{i=1}^\infty \mathbb{R}</math>, the infinite direct product and direct sum of the real numbers. Only sequences with a finite number of non-zero elements are in ''Y''. For example, (1,0,0,0,...) is in ''Y'' but (1,1,1,1,...) is not. Both of these sequences are in the direct product ''X''; in fact, ''Y'' is a proper subset of ''X'' (that is, ''Y''&nbsp;⊂&nbsp;''X'').
{{math|''f'' {{=}} {{sfrac|''c'' + 0|''c'' - ''c''}} ''f''{{sub|0}} {{=}} &infin; }}
and an observer behind the source will hear a lower frequency
{{math|''f'' {{=}} {{sfrac|''c'' - 0|''c'' + ''c''}} ''f''{{sub|0}} {{=}} 0.5 ''f''{{sub|0}} }}.


|File:Dopplereffectsourcemovingrightatmach1.4.gif|alt4=|The sound source has now broken through the sound speed barrier, and is traveling at 1.4 ''c'' (Mach 1.4). Since the source is moving faster than the sound waves it creates, it actually leads the advancing wavefront. The sound source will pass by a stationary observer before the observer hears the sound. As a result, an observer in front of the source will detect
== Topological space direct product ==
{{math|''f'' {{=}} {{sfrac|''c'' + 0|''c'' - 1.4''c''}} ''f''{{sub|0}} {{=}} -2.5 ''f''{{sub|0}} }}
The direct product for a collection of [[topological space]]s ''X<sub>i</sub>'' for ''i'' in ''I'', some index set, once again makes use of the Cartesian product
and an observer behind the source will hear a lower frequency
{{math|''f'' {{=}} {{sfrac|''c'' - 0|''c'' + 1.4''c''}} ''f''{{sub|0}} {{=}} 0.42 ''f''{{sub|0}} }}.
}}


==Analysis==
:<math>\prod_{i \in I} X_i. </math>
The frequency of the sounds that the source ''emits'' does not actually change. To understand what happens, consider the following analogy. Someone throws one ball every second in a man's direction. Assume that balls travel with constant velocity. If the thrower is stationary, the man will receive one ball every second. However, if the thrower is moving towards the man, he will receive balls more frequently because the balls will be less spaced out. The inverse is true if the thrower is moving away from the man. So it is actually the ''wavelength'' which is affected; as a consequence, the received frequency is also affected. It may also be said that the velocity of the wave remains constant whereas wavelength changes; hence frequency also changes. Note that in the ball analogy, the speed of the balls is dependent on the speeds of the thrower and receiver which is not the case of the wavefront velocity which remains constant.


With an observer stationary relative to the medium, if a moving source is emitting waves with an actual frequency <math>f_\text{0}</math> (in this case, the wavelength is changed, the transmission velocity of the wave keeps constant <math>\text{--}</math> note that the ''transmission velocity'' of the wave does not depend on the ''velocity of the source''), then the observer detects waves with a frequency <math>f</math> given by
Defining the [[topology]] is a little tricky. For finitely many factors, this is the obvious and natural thing to do: simply take as a [[basis (topology)|basis]] of open sets to be the collection of all cartesian products of open subsets from each factor:


:<math>f = \left ( \frac {c}{c + v_\text{s}} \right ) f_0</math>
:<math>\mathcal B = \{ U_1 \times \cdots \times U_n\ |\ U_i\ \mathrm{open\ in}\ X_i \}.</math>


A similar analysis for a moving ''observer'' and a stationary source (in this case, the wavelength keeps constant, but due to the motion, the rate at which the observer receives waves <math>\text{--}</math> and hence the ''transmission velocity'' of the wave [with respect to the observer] <math>\text{--}</math> is changed) yields the observed frequency:
This topology is called the [[product topology]]. For example, directly defining the product topology on '''R'''<sup>2</sup> by the open sets of '''R''' (disjoint unions of open intervals), the basis for this topology would consist of all disjoint unions of open rectangles in the plane (as it turns out, it coincides with the usual [[metric space|metric]] topology).


:<math>f = \left ( \frac {c + v_\text{r}}{c} \right ) f_0</math>
The product topology for infinite products has a twist, and this has to do with being able to make all the projection maps continuous and to make all functions into the product  continuous if and only if all its component functions are continuous (i.e. to satisfy the categorical definition of product: the morphisms here are continuous functions): we take as a basis of open sets to be the collection of all cartesian products of open subsets from each factor, as before, with the proviso that all but finitely many of the open subsets are the entire factor:


These can be generalized into the equation that was presented in the previous section.
:<math>\mathcal B = \left\{ \prod_{i \in I} U_i\ \Big|\ (\exists j_1,\ldots,j_n)(U_{j_i}\ \mathrm{open\ in}\ X_{j_i})\ \mathrm{and}\ (\forall i \neq j_1,\ldots,j_n)(U_i = X_i) \right\}.</math>


:<math>f = \left ( \frac {c+v_\text{r}}{c + v_\text{s}} \right ) f_0</math><center>
The more natural-sounding topology would be, in this case, to take products of infinitely many open subsets as before, and this does yield a somewhat interesting topology, the [[box topology]]. However it is not too difficult to find an example of bunch of continuous component functions whose product function is not continuous (see the separate entry box topology for an example and more). The problem which makes the twist necessary is ultimately rooted in the fact that the intersection of open sets is only guaranteed to be open for finitely many sets in the definition of topology.


An interesting effect was predicted by Lord Rayleigh in his classic book on sound: if the source is moving at twice the speed of sound, a musical piece emitted by that source would be heard in correct time and tune, but ''backwards''.<ref>{{cite book|last=Strutt (Lord Rayleigh)|first=John William|title=The Theory of Sound|editor=MacMillan & Co|date=1896|edition=2|volume=2|pages=154|url=http://archive.org/stream/theorysound02raylgoog#page/n176/mode/2up}}</ref>
Products (with the product topology) are nice with respect to preserving properties of their factors; for example, the product of Hausdorff spaces is Hausdorff; the product of connected spaces is connected, and the product of compact spaces is compact. That last one, called [[Tychonoff's theorem]], is yet another equivalence to the [[axiom of choice]].


==Application==
For more properties and equivalent formulations, see the separate entry [[product topology]].


===Sirens===
== Direct product of binary relations ==
The [[siren (noisemaker)|siren]] on a passing [[emergency vehicle]] will start out higher than its stationary pitch, slide down as it passes, and continue lower than its stationary pitch as it recedes from the observer. Astronomer [[John Dobson (astronomer)|John Dobson]] explained the effect thus:
On the Cartesian product of two sets with [[binary relation]]s ''R'' and ''S'', define (''a'', ''b'') T (''c'', ''d'') as ''a'' ''R'' ''c'' and ''b'' ''S'' ''d''. If ''R'' and ''S'' are both [[reflexive relation|reflexive]], [[irreflexive relation|irreflexive]], [[transitive relation|transitive]], [[symmetric relation|symmetric]], or [[antisymmetric relation|antisymmetric]], relation ''T'' has the same property.<ref>[http://cr.yp.to/2005-261/bender1/EO.pdf Equivalence and Order]</ref> Combining properties it follows that this also applies for being a [[preorder]] and being an [[equivalence relation]]. However, if ''R'' and ''S'' are [[total relation]]s, ''T'' is in general not.


:"The reason the siren slides is because it doesn't hit you."
== Categorical product ==
{{Main|Product (category theory)}}


In other words, if the siren approached the observer directly, the pitch would remain constant until the vehicle hit him, and then immediately jump to a new lower pitch. Because the vehicle passes by the observer, the radial velocity does not remain constant, but instead varies as a function of the angle between his line of sight and the siren's velocity:
The direct product can be abstracted to an arbitrary [[category theory|category]]. In a general category, given a collection of objects ''A<sub>i</sub>'' ''and'' a collection of [[morphism]]s ''p<sub>i</sub>'' from ''A'' to ''A<sub>i</sub>''{{clarify|Is A a single object from A_i, or all A_i?|date=February 2012}} with ''i'' ranging in some index set ''I'', an object ''A'' is said to be a '''categorical product''' in the category if, for any object ''B'' and any collection of morphisms ''f<sub>i</sub>'' from ''B'' to ''A<sub>i</sub>'', there exists a unique morphism ''f'' from ''B'' to ''A'' such that ''f<sub>i</sub> = p<sub>i</sub> f'' and this object ''A'' is unique. This not only works for two factors, but arbitrarily (even infinitely) many.


:<math>v_\text{radial}=v_\text{s}\cdot \cos{\theta}</math>
For groups we similarly define the direct product of a more general, arbitrary collection of groups ''G<sub>i</sub>'' for ''i'' in ''I'', ''I'' an index set. Denoting the cartesian product of the groups by ''G'' we define multiplication on ''G''  with the operation of componentwise multiplication; and corresponding to the ''p<sub>i</sub>'' in the definition above are the projection maps


where <math>\theta</math> is the angle between the object's forward velocity and the line of sight from the object to the observer.
:<math>\pi_i \colon G \to G_i\quad \mathrm{by} \quad \pi_i(g) = g_i</math>,


===Astronomy===
the functions that take <math>(g_j)_{j \in I}</math> to its ''i''th component ''g<sub>i</sub>''.
[[Image:Redshift.svg|thumb|200px|[[Redshift]] of [[spectral line]]s in the [[optical spectrum]] of a supercluster of distant galaxies (right), as compared to that of the Sun (left)]]
<!-- this is easier to visualize as a [[commutative diagram]]; eventually somebody should insert a relevant diagram for the categorical product here! -->


The Doppler effect for [[electromagnetic waves]] such as light is of great use in [[astronomy]] and results in either a so-called [[redshift]] or [[blueshift]]. It has been used to measure the speed at which [[star]]s and [[galaxy|galaxies]] are approaching or receding from us, that is, the [[radial velocity]]. This is used to detect if an apparently single star is, in reality, a close [[Binary star|binary]] and even to measure the rotational speed of stars and galaxies.
== Internal and external direct product ==
<!-- linked from [[Internal direct product]] and [[External direct product]] -->
{{see also|Internal direct sum}}


The use of the Doppler effect for light in [[astronomy]] depends on our knowledge that the [[electromagnetic spectroscopy|spectra]] of stars are not homogeneous. They exhibit [[spectral line|absorption lines]] at well defined frequencies that are correlated with the energies required to excite [[electron]]s in various [[Chemical element|elements]] from one level to another. The Doppler effect is recognizable in the fact that the absorption lines are not always at the frequencies that are obtained from the spectrum of a stationary light source. Since blue light has a higher frequency than red light, the spectral lines of an approaching astronomical light source exhibit a blueshift and those of a receding astronomical light source exhibit a redshift.
Some authors draw a distinction between an '''internal direct product''' and an '''external direct product.''' If <math>A, B \subset X</math> and <math>A \times B \cong X</math>, then we say that ''X'' is an ''internal'' direct product (of ''A'' and ''B''); if ''A'' and ''B'' are not subobjects, then we say that this is an ''external'' direct product.


Among the [[List of nearest stars|nearby stars]], the largest radial velocities with respect to the [[Sun]] are +308&nbsp;km/s ([[BD-15°4041]], also known as LHS 52, 81.7 light-years away) and -260&nbsp;km/s ([[Woolley 9722]], also known as Wolf 1106 and LHS 64, 78.2 light-years away). Positive radial velocity means the star is receding from the Sun, negative that it is approaching.
==Metric and norm==
A metric on a Cartesian product of metric spaces, and a norm on a direct product of normed vector spaces, can be defined in various ways, see for example [[Norm_%28mathematics%29#p-norm|p-norm]].


===Radar===
==See also==
{{Main|Doppler radar}}
*[[Direct sum]]
 
*[[Cartesian product]]
The Doppler effect is used in some types of [[radar]], to measure the velocity of detected objects. A radar beam is fired at a moving target — e.g. a motor car, as police use radar to detect speeding motorists — as it approaches or recedes from the radar source. Each successive radar wave has to travel farther to reach the car, before being reflected and re-detected near the source. As each wave has to move farther, the gap between each wave increases, increasing the wavelength. In some situations, the radar beam is fired at the moving car as it approaches, in which case each successive wave travels a lesser distance, decreasing the wavelength. In either situation, calculations from the Doppler effect accurately determine the car's velocity taking into account wind speed and direction relative to the car. Moreover, the [[proximity fuze]], developed during World War II, relies upon Doppler radar to detonate explosives at the correct time, height, distance, etc.{{Citation needed|date=December 2009}}
*[[Coproduct]]
 
*[[Free product]]
===Medical imaging and blood flow measurement===
*[[Semidirect product]]
[[File:CarotidDoppler1.jpg|thumb||200px|Colour flow ultrasonography (Doppler) of a [[carotid artery]] - scanner and screen]]
*[[Zappa–Szep product]]
An [[echocardiogram]] can, within certain limits, produce an accurate assessment of the direction of blood flow and the velocity of blood and cardiac tissue at any arbitrary point using the Doppler effect. One of the limitations is that the [[ultrasound]] beam should be as parallel to the blood flow as possible. Velocity measurements allow assessment of cardiac valve areas and function, any abnormal communications between the left and right side of the heart, any leaking of blood through the valves (valvular regurgitation), and calculation of the [[cardiac output]]. [[Contrast-enhanced ultrasound]] using gas-filled microbubble contrast media can be used to improve velocity or other flow-related medical measurements.
*[[Tensor product of graphs]]
 
*[[Total_order#Orders_on_the_Cartesian_product_of_totally_ordered_sets|Orders on the Cartesian product of totally ordered sets]]
Although "Doppler" has become synonymous with "velocity measurement" in medical imaging, in many cases it is not the frequency shift (Doppler shift) of the received signal that is measured, but the phase shift (''when'' the received signal arrives).
 
Velocity measurements of blood flow are also used in other fields of [[medical ultrasonography]], such as [[obstetric ultrasonography]] and [[neurology]]. Velocity measurement of blood flow in arteries and veins based on Doppler effect is an effective tool for diagnosis of vascular problems like stenosis.<ref>{{cite book |first=D. H. |last=Evans |first2=W. N. |last2=McDicken |title=Doppler Ultrasound |edition=Second |publisher=John Wiley and Sons |location=New York |date=2000 |isbn=0-471-97001-8 }}</ref>
 
===Flow measurement===
Instruments such as the [[laser Doppler velocimetry|laser Doppler velocimeter]] (LDV), and [[acoustic Doppler velocimetry|acoustic Doppler velocimeter]] (ADV) have been developed to measure [[velocity|velocities]] in a fluid flow. The LDV emits a light beam and the ADV emits an ultrasonic acoustic burst, and measure the Doppler shift in wavelengths of reflections from particles moving with the flow. The actual flow is computed as a function of the water velocity and phase. This technique allows non-intrusive flow measurements, at high precision and high frequency.
 
===Velocity profile measurement===
Developed originally for velocity measurements in medical applications (blood flow), Ultrasonic Doppler Velocimetry (UDV) can measure in real time complete velocity profile in almost any liquids containing particles in suspension such as dust, gas bubbles, emulsions. Flows can be pulsating, oscillating, laminar or turbulent, stationary or transient. This technique is fully non-invasive.


===Satellite communication===
== Notes ==
Fast moving satellites can have a Doppler shift of dozens of kilohertz relative to a ground station. The speed, thus magnitude of Doppler effect, changes due to earth curvature. Dynamic Doppler compensation, where the frequency of a signal is changed multiple times during transmission, is used so the satellite receives a constant frequency signal.<ref>{{Citation |last=Qingchong |first=Liu |title=Doppler measurement and compensation in mobile satellite communications systems |journal=Military Communications Conference Proceedings / MILCOM |volume=1 |date=1999 |pages=316–320 |url=http://ieeexplore.ieee.org/xpl/freeabs_all.jsp?arnumber=822695 |doi=10.1109/milcom.1999.822695}}</ref>
<references />
 
===Audio===
The [[Leslie speaker]], associated with and predominantly used with the [[Hammond organ|Hammond B-3 organ]], takes advantage of the Doppler Effect by using an electric motor to rotate an acoustic horn around a loudspeaker, sending its sound in a circle. This results at the listener's ear in rapidly fluctuating frequencies of a keyboard note.
 
===Vibration measurement===
A [[laser Doppler vibrometer]] (LDV) is a non-contact method for measuring vibration. The laser beam from the LDV is directed at the surface of interest, and the vibration amplitude and frequency are extracted from the Doppler shift of the laser beam frequency due to the motion of the surface.
 
{{Listen|filename=Speeding-car-horn_doppler_effect_sample.ogg|title=Passing car horn|format=[[Ogg]]}}
 
==Inverse Doppler effect==
Since 1968 Scientists such as [[Victor Veselago]] have speculated about the possibility of an Inverse Doppler effect. An experiment that claimed to have detected this effect was conducted by Nigel Seddon and Trevor Bearpark in [[Bristol]], [[United Kingdom]] in 2003.<ref>{{citation|
title=The Inverse Doppler effect: Researchers add to the bylaws of physics|
publisher=physorg.com|
date=May 23, 2005|
accessdate=2008-03-08|
url=http://www.physorg.com/news4224.html}}</ref>
 
Researchers from [[Swinburne University of Technology]] and the [[University of Shanghai for Science and Technology]] showed that this effect can be observed in optical frequencies as well. This was made possible by growing a [[photonic crystal]] and projecting a laser beam into the crystal. This made the crystal act like a [[superprism|super prism]] and the Inverse Doppler Effect could be observed.<ref>{{citation|
title=Scientists reverse Doppler Effect|
publisher=physorg.com|
date=March 7, 2011|
accessdate=2011-03-18|
url=http://www.physorg.com/news/2011-03-scientists-reverse-doppler-effect.html}}</ref>
 
==See also==
* [[Relativistic Doppler effect]]
* [[Dopplergraph]]
* [[Fizeau experiment]]
* [[Fading]]
* [[Photoacoustic Doppler effect]]
* [[Differential Doppler effect]]
* [[Rayleigh fading]]


== References ==
== References ==
{{reflist}}
*{{Lang Algebra}}
 
==Further reading==
* Doppler, C. J. (1842). ''[[Über das farbige Licht der Doppelsterne und einiger anderer Gestirne des Himmels|Über das farbige Licht der Doppelsterne und einiger anderer Gestirne des Himmels (About the coloured light of the binary stars and some other stars of the heavens)]]''. Publisher: Abhandlungen der Königl. Böhm. Gesellschaft der Wissenschaften (V. Folge, Bd. 2, S. 465-482) [Proceedings of the Royal Bohemian Society of Sciences (Part V, Vol 2)]; Prague: 1842 (Reissued 1903). Some sources mention 1843 as year of publication because in that year the article was published in the Proceedings of the Bohemian Society of Sciences. Doppler himself referred to the publication as "Prag 1842 bei Borrosch und André", because in 1842 he had a preliminary edition printed that he distributed independently.
* "Doppler and the Doppler effect", E. N. da C. Andrade, ''Endeavour'' Vol. XVIII No. 69, January 1959 (published by ICI London). Historical account of Doppler's original paper and subsequent developments.
* {{cite web | url = http://archive.ncsa.uiuc.edu/Cyberia/Bima/doppler.html | title = Doppler Effect | first = Eleni | last = Adrian | publisher = [[National Center for Supercomputing Applications|NCSA]] | date = 24 June 1995 | accessdate = 2008-07-13 }}


==External links==
{{DEFAULTSORT:Direct Product}}
{{Commons}}
[[Category:Abstract algebra]]
* [http://scienceworld.wolfram.com/physics/DopplerEffect.html Doppler Effect], [ScienceWorld]
* [http://www.falstad.com/ripple/ex-doppler.html Java simulation of Doppler effect]
* [http://www.mathpages.com/rr/s2-04/2-04.htm Doppler Shift for Sound and Light] at MathPages
* [http://scratch.mit.edu/projects/12532039/ Flash simulation and game of Doppler effect of sound] at [[Scratch (programming language)]]
* [http://www.kettering.edu/~drussell/Demos/doppler/doppler.html The Doppler Effect and Sonic Booms (D.A. Russell, Kettering University)]
* [http://beta.vtap.com/video/Doppler+Effect/CL0113709540_1d645df0e Video Mashup with Doppler Effect videos]
* [http://math.ucr.edu/~jdp/Relativity/WaveDancer.html Wave Propagation] ''from John de Pillis.'' An animation showing that the speed of a moving wave source does not affect the speed of the wave.
* [http://math.ucr.edu/~jdp/Relativity/EM_Propagation.html EM Wave Animation] ''from John de Pillis.'' How an electromagnetic wave propagates through a vacuum
* [http://astro.unl.edu/classaction/animations/light/dopplershift.html Doppler Shift Demo] - Interactive flash simulation for demonstrating Doppler shift.
*[http://www.colorado.edu/physics/2000/applets_New.html Interactive applets] at Physics 2000


{{DEFAULTSORT:Doppler Effect}}
[[ru:Прямое произведение#Прямое произведение групп]]
[[Category:Doppler effects]]
[[Category:Radio frequency propagation]]
[[Category:Wave mechanics]]
[[Category:Radar signal processing]]

Revision as of 12:31, 8 August 2014

In mathematics, one can often define a direct product of objects already known, giving a new one. This generalizes the Cartesian product of the underlying sets, together with a suitably defined structure on the product set. More abstractly, one talks about the product in category theory, which formalizes these notions.

Examples are the product of sets (see Cartesian product), groups (described below), the product of rings and of other algebraic structures. The product of topological spaces is another instance.

There is also the direct sum – in some areas this is used interchangeably, in others it is a different concept.

Examples

In a similar manner, we can talk about the product of more than two objects, e.g. . We can even talk about product of infinitely many objects, e.g. .

Group direct product

Mining Engineer (Excluding Oil ) Truman from Alma, loves to spend time knotting, largest property developers in singapore developers in singapore and stamp collecting. Recently had a family visit to Urnes Stave Church. In group theory one can define the direct product of two groups (G, *) and (H, ●), denoted by G × H. For abelian groups which are written additively, it may also be called the direct sum of two groups, denoted by .

It is defined as follows:

  • the set of the elements of the new group is the cartesian product of the sets of elements of G and H, that is {(g, h): g in G, h in H};
  • on these elements put an operation, defined elementwise:
    (g, h) × (g' , h' ) = (g * g' , hh' )

(Note the operation * may be the same as ●.)

This construction gives a new group. It has a normal subgroup isomorphic to G (given by the elements of the form (g, 1)), and one isomorphic to H (comprising the elements (1, h)).

The reverse also holds, there is the following recognition theorem: If a group K contains two normal subgroups G and H, such that K= GH and the intersection of G and H contains only the identity, then K is isomorphic to G x H. A relaxation of these conditions, requiring only one subgroup to be normal, gives the semidirect product.

As an example, take as G and H two copies of the unique (up to isomorphisms) group of order 2, C2: say {1, a} and {1, b}. Then C2×C2 = {(1,1), (1,b), (a,1), (a,b)}, with the operation element by element. For instance, (1,b)*(a,1) = (1*a, b*1) = (a,b), and (1,b)*(1,b) = (1,b2) = (1,1).

With a direct product, we get some natural group homomorphisms for free: the projection maps

,

called the coordinate functions.

Also, every homomorphism f to the direct product is totally determined by its component functions .

For any group (G, *), and any integer n ≥ 0, multiple application of the direct product gives the group of all n-tuples Gn (for n = 0 the trivial group). Examples:

Direct product of modules

The direct product for modules (not to be confused with the tensor product) is very similar to the one defined for groups above, using the cartesian product with the operation of addition being componentwise, and the scalar multiplication just distributing over all the components. Starting from R we get Euclidean space Rn, the prototypical example of a real n-dimensional vector space. The direct product of Rm and Rn is Rm + n.

Note that a direct product for a finite index is identical to the direct sum . The direct sum and direct product differ only for infinite indices, where the elements of a direct sum are zero for all but for a finite number of entries. They are dual in the sense of category theory: the direct sum is the coproduct, while the direct product is the product.

For example, consider and , the infinite direct product and direct sum of the real numbers. Only sequences with a finite number of non-zero elements are in Y. For example, (1,0,0,0,...) is in Y but (1,1,1,1,...) is not. Both of these sequences are in the direct product X; in fact, Y is a proper subset of X (that is, Y ⊂ X).

Topological space direct product

The direct product for a collection of topological spaces Xi for i in I, some index set, once again makes use of the Cartesian product

Defining the topology is a little tricky. For finitely many factors, this is the obvious and natural thing to do: simply take as a basis of open sets to be the collection of all cartesian products of open subsets from each factor:

This topology is called the product topology. For example, directly defining the product topology on R2 by the open sets of R (disjoint unions of open intervals), the basis for this topology would consist of all disjoint unions of open rectangles in the plane (as it turns out, it coincides with the usual metric topology).

The product topology for infinite products has a twist, and this has to do with being able to make all the projection maps continuous and to make all functions into the product continuous if and only if all its component functions are continuous (i.e. to satisfy the categorical definition of product: the morphisms here are continuous functions): we take as a basis of open sets to be the collection of all cartesian products of open subsets from each factor, as before, with the proviso that all but finitely many of the open subsets are the entire factor:

The more natural-sounding topology would be, in this case, to take products of infinitely many open subsets as before, and this does yield a somewhat interesting topology, the box topology. However it is not too difficult to find an example of bunch of continuous component functions whose product function is not continuous (see the separate entry box topology for an example and more). The problem which makes the twist necessary is ultimately rooted in the fact that the intersection of open sets is only guaranteed to be open for finitely many sets in the definition of topology.

Products (with the product topology) are nice with respect to preserving properties of their factors; for example, the product of Hausdorff spaces is Hausdorff; the product of connected spaces is connected, and the product of compact spaces is compact. That last one, called Tychonoff's theorem, is yet another equivalence to the axiom of choice.

For more properties and equivalent formulations, see the separate entry product topology.

Direct product of binary relations

On the Cartesian product of two sets with binary relations R and S, define (a, b) T (c, d) as a R c and b S d. If R and S are both reflexive, irreflexive, transitive, symmetric, or antisymmetric, relation T has the same property.[1] Combining properties it follows that this also applies for being a preorder and being an equivalence relation. However, if R and S are total relations, T is in general not.

Categorical product

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The direct product can be abstracted to an arbitrary category. In a general category, given a collection of objects Ai and a collection of morphisms pi from A to AiTemplate:Clarify with i ranging in some index set I, an object A is said to be a categorical product in the category if, for any object B and any collection of morphisms fi from B to Ai, there exists a unique morphism f from B to A such that fi = pi f and this object A is unique. This not only works for two factors, but arbitrarily (even infinitely) many.

For groups we similarly define the direct product of a more general, arbitrary collection of groups Gi for i in I, I an index set. Denoting the cartesian product of the groups by G we define multiplication on G with the operation of componentwise multiplication; and corresponding to the pi in the definition above are the projection maps

,

the functions that take to its ith component gi.

Internal and external direct product

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Some authors draw a distinction between an internal direct product and an external direct product. If and , then we say that X is an internal direct product (of A and B); if A and B are not subobjects, then we say that this is an external direct product.

Metric and norm

A metric on a Cartesian product of metric spaces, and a norm on a direct product of normed vector spaces, can be defined in various ways, see for example p-norm.

See also

Notes

References

ru:Прямое произведение#Прямое произведение групп