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Tisa (berg i Makedonien, lat 41,66, long 22,10)

September 15th, 2017

Tisa (makedonska: Тиса) är ett berg i Makedonien. Det ligger i den centrala delen av landet, 70 kilometer sydost om huvudstaden Skopje. Toppen på Tisa är 653 meter över havet, eller 126 meter över den omgivande terrängen. Bredden vid basen är 1,9 km.

Terrängen runt Tisa är huvudsakligen kuperad, men norrut är den platt buy football t shirts. Den högsta punkten i närheten är Sjtrkalevo, 711 meter över havet, 2,0 kilometer sydost om Tisa. Närmaste större samhälle är Štip quick meat tenderizer, 12,2 kilometer nordost om Tisa. I trakten runt Tisa finns ovanligt många namngivna kullar och klippformationer.

Trakten runt Tisa består i huvudsak av gräsmarker. Runt Tisa är det ganska tätbefolkat, med 83 invånare per kvadratkilometer

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. Trakten ingår i den hemiboreala klimatzonen. Årsmedeltemperaturen i trakten är 14 °C. Den varmaste månaden är juli, då medeltemperaturen är 28 °C, och den kallaste är januari, med 0 °C. Genomsnittlig årsnederbörd är 1 028 millimeter. Den regnigaste månaden är februari, med i genomsnitt 132 mm nederbörd electric lint remover, och den torraste är augusti, med 37 mm nederbörd.

Mont Pinçon

September 15th, 2017

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Géolocalisation sur la carte : Calvados

Géolocalisation sur la carte : France

Le mont Pinçon est le plus haut point du département du Calvados en Normandie avec une altitude de 362 mètres good soccer goalies. Il est situé à l’ouest de la Suisse normande à une trentaine de kilomètres au sud-ouest de Caen, près du village du Plessis-Grimoult.

Pendant l’Occupation, les Allemands y installent un poste de radioguidage à ondes courtes Knickebein pour le guidage des avions de la Luftwaffe, ainsi qu’une tour d’observation. Pendant la bataille de Normandie, lors de l’opération Bluecoat, les Alliés approchent du mont. La 43e division d’infanterie Wessex britannique tente de s’en emparer le 5 août 1944 mais subit un échec lors de son passage par Saint-Jean-le-Blanc. Le lendemain une attaque est tentée en passant plus au nord après une préparation d’artillerie mais elle est bloquée par des troupes des 276e et 326e divisions d’infanterie allemande. C’est finalement un escadron de chars Sherman M4 du 13/18th Royal Hussars, mené par le major Denny qui réussit à atteindre le sommet sous couvert de fumigènes. Ils sont rejoints dans la nuit par l’infanterie du 4th Somerset et du 4th Wiltshire. Les tentatives allemandes pour reprendre le mont les jours suivants n’aboutissent pas.

En 1956, la RTF installe un émetteur sur un pylône de plus de 200 mètres de haut. À la fin des années 1960 runners water bottle holder, ce pylône est démonté et remplacé par un pylône de type tubulaire de 216 mètres de haut qui permet la diffusion de la télévision (TNT) et des radios de Radio France en FM sur la majeure partie de la Basse-Normandie. Le pylône culmine ainsi à 578 mètres d’altitude best steak marinade tenderizer.

Installation TDF.

Monument aux Royal Hussars.

Sur les autres projets Wikimedia :

Kirchlein

September 15th, 2017

Lage von Kirchlein in Bayern

Kirchlein ist ein Kirchdorf mit 188 Einwohnern und Ortsteil von Burgkunstadt im oberfränkischen Landkreis Lichtenfels im Norden des Freistaates Bayern.

Kirchlein liegt auf 355–382 m ü tenderizing a steak. NN am nördlichen Ende des Häckergrundes, durch den der Häckergrundbach fließt. Die amtliche Höhe wird mit m&nbsp

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;ü. NN angegeben. Südlich des Dorfes liegt der Fleckberg (400,6 m ü. NHN), im Westen der Spitzberg (517,6 m ü. NHN). Der Ort gehört noch zum Obermainischen Bruchschollenland. Der Ortskern von Burgkunstadt befindet sich etwa 4,5 Kilometer südwestlich.

Wann Kirchlein gegründet wurde, ist unbekannt. Eventuell könnte die Siedlung in ihrer Frühform bereits als Einzelhof oder befestigter Vorhof im 9. Jahrhundert n. Chr. entstanden sein und der Burg cunstat unterstanden haben (siehe dazu: Geschichte der Stadt Burgkunstadt#8. Jahrhundert bis 1058: erste Siedlungsanfänge). Erstmals gesichert wird von der Ortschaft um 1330 in zwei Urbaren des Klosters Langheim, bezüglich zweier Flurverkäufe durch „Albert […] aus Gleind“ berichtet. In Urkunden aus dem frühen Mittelalter wird der Ort bereits mehrmals bis 1490 als „Gleind“ oder „Kirchgleind“ erwähnt. Die ältere Form Gleind wurde jedoch seltener gebraucht. Die Vorsilbe Kirch könnte sich einerseits auf den Bau der Kirche beziehen, andererseits aber auch nur zur Unterscheidung von anderen Dörfern gleichen Namens gedient haben. Die Silbe -lein, -glein bzw. -gleind wurde früher oftmals als Abwandlung von Gelände verwendet. Inzwischen gilt jedoch als gesichert, dass die Silbe vom slawischen Wort glina für Lehm herrührt, der häufig in den Fluren um Kirchlein vorkommt.

Die örtliche Pfarrei gehörte jahrhundertelang zu Altenkunstadt. Am 24. November 1477 wurde Kirchlein zu einer eigenen Pfarrei erhoben. Der Dreißigjährige Krieg hinterließ in Kirchlein große Schäden. An die Erschlagung zweier schwedischer Soldaten durch Kirchleiner Bürger erinnert die Schwedenlinde auf der Anhöhe Kalte Staude.

Die Alte Pfarrkirche um 1900

Südwestansicht von Kirchlein um 1920

Postkarte des Dorfplatzes von Kirchlein um 1920. Gut zu sehen ist in der Bildmitte der Nachfolgebau der alten Pfarrkirche

Die Tiefe Gasse vor dem Ausbau (um 1910)

Die alte romanische Kirche wurde 1905/1906 abgerissen und anschließend an derselben Stelle eine neue errichtet. Anders als der Vorgängerbau erinnert sie mehr an die Gotik. Das ehemalige Schulhaus neben der Kirche wurde 1925 errichtet und wurde bis in die 1960er Jahre benutzt. Die Ortsdurchfahrt Tiefe Gasse wurde zwischen Juni und November 1939 ausgebaut und saniert.

Am 10. Mai 1971 wurde der FC Kirchlein gegründet. Mit der Eintragung in das Vereinsregister erhielt der Verein 1978 den heutigen Namen 1. FC Kirchlein e. V. In den folgenden Jahren fanden zahlreiche Baumaßnahmen am Sportplatz statt. Das Sportlerheim wurde in Eigenleistung des Vereins in den Jahren 1988/1989 gebaut.

Am 1. Januar 1977 wurde Kirchlein, das bis dahin zusammen mit Hainzendorf und Reuth eine eigenständige Gemeinde gebildet hatte, nach Burgkunstadt eingemeindet.

Die Tabelle gibt die Einwohnerentwicklung Kirchleins wieder.

Burgkunstadt | Eben | Ebneth | Flurholz | Gärtenroth | Hainweiher | Hainzendorf | Kaltenreuth | Kirchlein | Lopphof | Mainklein | Mainroth | Meuselsberg | Neue Weiher | Neuses | Pfaffeggetten | Reuth | Theisau | Weidnitz | Wildenroth

Fakultativer Unterricht

September 15th, 2017

Der fakultative Unterricht ist ein Angebot für besonders begabte Schüler. Es ist zusätzlicher und freiwilliger Unterricht in bestimmten Fächern running water bottle belt reviews.

Fakultativen Unterricht gibt es zum Beispiel an der KSOe in der Schweiz und am Deutsch-Französischen Gymnasium in Saarbrücken personalized toddler water bottles.

Der fakultative Unterricht war auch eine Unterrichtsform in der DDR. Er fand außerhalb der normalen Unterrichtszeit statt und war freiwillig. Nach der Entscheidung für einen oder mehrere fakultative Kurse waren diese verpflichtender Unterricht. Die Anwesenheit wurde kontrolliert. Die Strenge der Umsetzung wurde von Schule zu Schule unterschiedlich gehandhabt. Am fakultativen Unterricht konnten Schüler aus verschiedenen Parallelklassen teilnehmen. Teilweise gab es bestimmte Mindestleistungen, die erreicht werden mussten, damit man am fakultativen Unterricht teilnehmen konnte. Das betraf hauptsächlich sehr begehrte fakultative Kurse, wie bspw. Informatik. Die Mindestvoraussetzungen waren demnach als ein Mittel zur Steuerung des Zulaufs an Teilnehmern zu bewerten.

Obligatorisch wurde zum Beispiel Russisch gelehrt. Dagegen fand der Englisch- bzw. Französisch-Unterricht in der POS als fakultativer Unterricht statt. Noten für fakultativen Sprachunterricht fanden sich auch auf den Jahresabschlusszeugnissen wieder, hatten aber keinen Einfluss auf die Versetzung. Welche zweite Fremdsprache als fakultativer Unterricht in der POS angeboten wurde, oblag der Schule. Schüler oder Eltern hatten darauf in der Regel keinen Einfluss. Hauptsächlich war es Englisch glass bottle of water, in einigen Fällen Französisch, selten Spanisch stainless steel toothpaste dispenser. In der EOS war eine zweite Fremdsprache dann ebenfalls obligatorisch.

Zusätzlich zu dem normalen Unterricht konnte man auch in einigen Fächern an fakultativem Unterricht auch in naturwissenschaftlichen Fächern teilnehmen, zum Beispiel in Mathematik an einem Kurs zum Thema der Komplexen Zahlen oder Chemie mit erweiterten Versuchsreihen in organischer Chemie. Die behandelten Themen richteten sich neben den pädagogischen Vorgaben auch an den Interessen der teilnehmenden Schüler.

In künstlerischen Fächern gab es den wahlobligatorischen Unterricht, wahlweise konnte man im 11. und 12. Schuljahr der EOS entweder am Musikunterricht oder an Kunsterziehung (Zeichnen) teilnehmen.

Nach der Wiedervereinigung gab es ähnliche Systeme zur Gestaltung des Unterrichts im Gymnasium in Form des Kurssystems.

Daniel Burley Woolfall

September 14th, 2017

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Daniel Burley Woolfall en 1908

Daniel Burley Woolfall bag for cell phone, né le à Blackburn et mort le , est un dirigeant britannique de football. Représentant de la Fédération d’Angleterre de football, il dirige également la FIFA de 1906 à sa mort en 1918.

Juriste international

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, Daniel Burley Woolfall est trésorier puis vice-président de la Fédération d’Angleterre de football alternative meat tenderizer.

Pendant son mandat à la tête de la FIFA eco friendly water bottles, il fait notamment adopter les lois du jeu maintenues par l’International Football Association Board (IFAB), accueille les premières nations non-européennes et impulse l’organisation du premier tournoi de football aux Jeux olympiques en 1908.

Haderslev Vor Frue Domsogn

September 14th, 2017

Haderslev Vor Frue Domsogn er et sogn i Haderslev Domprovsti (Haderslev Stift). Sognet ligger i Haderslev Kommune og indtil kommunalreformen i 1970 lå det i Haderslev Herred (Haderslev Amt). I Haderslev Vor Frue Domsogn ligger Haderslev Domkirke og Hertug Hans Hospitalskirke.

I Haderslev Vor Frue Domsogn findes flg. autoriserede stednavne:

Domsognet omfatter den største del af Haderslev (2004: 13.673 indbyggere) og betjenes af en domprovst og fire sognepræster (heraf én for den tysksprogede del af menigheden) winter goalkeeper gloves. Foruden i Haderslev Domkirke, holdes der hver søn- og helligdag også gudstjeneste i Hertug Hans Hospitalskirke. Menighedsrådet har femten valgte medlemmer (i øjeblikket er to af disse valgt på en tysk liste) og bestyrer foruden kirkerne Assistens kirkegård i byens sydlige del. Under menighedsrådet er ansat et stort personale, bl.a. tre organister, kordegn, kirkegårdsleder, fire kirketjenere og en sognemedhjælper.

Ved genforeningen i 1920 fortsatte sognepræsten ved Domkirken som sognepræst for den tysksprogede del af menigheden og der oprettedes en sideordnet sognepræstestilling for den dansksprogede del af menigheden. Herefter skulle alle (dåbs- og vielses-) attester underskrives af begge sognepræster, hvilket hurtigt viste sig at være upraktisk, hvorfor det blev praksis, at Domsognets kordegn kunne underskrive. Denne ordning blev først senere udbredt til andre store sogne i folkekirken.

Koordinater:

Michael Wiseman

September 13th, 2017

Michael Wiseman (born April 12 toothpaste dispenser uk, 1967)[citation needed] is an American television and film actor. He is best known for his portrayal of Johnny Rizzo in the 2012 CBS series Vegas.

Wiseman grew up in Lafayette, California monogrammed football shirts. He knew as a boy that he wanted to be an actor; the caption of his eighth grade yearbook picture said, “Career Goal: football player or famous actor”. He graduated from Saint Mary’s College High School in Berkeley, California, in 1985.

Wiseman spent two decades working in Hollywood before landing the part of Rizzo, during which he played an outspoken student in the PBS series French in Action, performed supporting roles in Tim Burton’s remake of Planet of the Apes and Surviving Gilligan’s Island. He has acted in over 65 television series, including Cheers, ER, Melrose Place, NYPD Blue, and The X-Files.

Wiseman is married to Caroline Keenan-Wiseman, an Emmy-nominated hairstylist and makeup artist authentic jerseys for sale. The couple have two daughters. In 2011, Wiseman and his family moved back to his childhood city of Lafayette, California bottle stainless steel.

Klein–Gordon equation

September 13th, 2017

The Klein–Gordon equation (Klein–Fock–Gordon equation or sometimes Klein–Gordon–Fock equation) is a relativistic wave equation, related to the Schrödinger equation. It is second order in space and time and manifestly Lorentz covariant. It is a quantized version of the relativistic energy–momentum relation. Its solutions include a quantum scalar or pseudoscalar field, a field whose quanta are spinless particles. Its theoretical relevance is similar to that of the Dirac equation. Electromagnetic interactions can be incorporated, forming the topic of scalar electrodynamics, but because common spinless particles like the pi mesons are unstable and also experience the strong interaction (with unknown interaction term in the Hamiltonian), the practical utility is limited.

The equation can be put into the form of a Schrödinger equation. In this form it is two coupled differential equations, each of first order in time. The solutions have two components, reflecting the charge degree of freedom in relativity. It admits a conserved quantity, but this is not positive definite. The wave function cannot therefore be interpreted as a probability amplitude. The conserved quantity is instead interpreted as electric charge and the norm squared of the wave function is interpreted as a charge density. The equation describes all spinless particles with positive, negative as well as zero charge. Within the Feynman–Stueckelberg interpretation, particles and antiparticles are treated mathematically as if they propagate forward and backward in time respectively, the advanced propagator (as opposed to the retarded propagator) is employed for antiparticles. Physically, all particles move forward in time.

Any solution of the free Dirac equation is componentwise a solution of the free Klein–Gordon equation.

The equation does not form the basis for a consistent quantum relativistic one-particle theory. There is no known such theory for particles of any spin. For full reconciliation of quantum mechanics with special relativity quantum field theory is needed, in which the Klein–Gordon equation reemerges as the equation obeyed by the components of all free quantum fields. In quantum field theory, the solutions of the free (noninteracting) versions of the original equations still play a role. They are needed to build the Hilbert space (Fock space) and to express quantum field by using complete sets (spanning sets of Hilbert space) of wave functions.

The Klein–Gordon equation with mass parameter





m




{\displaystyle m}


is

Solutions of the equation are complex-valued functions





ψ



(


t


,




x




)




{\displaystyle \psi (t,{\mathbf {x}})}


of the time variable





t




{\displaystyle t}


and space variables







x






{\displaystyle {\mathbf {x}}}


; the Laplacian











2






{\displaystyle \nabla ^{2}}


acts on the space variables only.

The equation is often abbreviated as

where μ = mc/ħ and is the d’Alembert operator, defined by

(We are using the (−, +, +, +) metric signature.)

The Klein–Gordon equation is often written in natural units:

The form of the Klein–Gordon equation is derived by requiring that plane wave solutions of the equation:

obey the energy momentum relation of special relativity:

Unlike the Schrödinger equation, the Klein–Gordon equation admits two values of ω for each k, one positive and one negative. Only by separating out the positive and negative frequency parts does one obtain an equation describing a relativistic wavefunction. For the time-independent case, the Klein–Gordon equation becomes

which is formally the same as the homogeneous screened Poisson equation.

The equation was named after the physicists Oskar Klein and Walter Gordon, who in 1926 proposed that it describes relativistic electrons. Other authors making similar claims in that same year were Vladimir Fock, Johann Kudar, Théophile de Donder and Frans-H. van den Dungen, and Louis de Broglie. Although it turned out that modeling the electron’s spin required the Dirac equation, the Klein–Gordon equation correctly describes the spinless relativisitic composite particles, like the pion. On July 4, 2012 CERN announced the discovery of the Higgs boson. Since the Higgs boson is a spin-zero particle, it is the first observed ostensibly elementary particle to be described by the Klein–Gordon equation. Further experimentation and analysis is required to discern whether the Higgs boson observed is that of the Standard Model, or a more exotic, possibly composite, form.

The Klein–Gordon equation was first considered as a quantum wave equation by Schrödinger in his search for an equation describing de Broglie waves. The equation is found in his notebooks from late 1925, and he appears to have prepared a manuscript applying it to the hydrogen atom. Yet, because it fails to take into account the electron’s spin, the equation predicts the hydrogen atom’s fine structure incorrectly, including overestimating the overall magnitude of the splitting pattern by a factor of 4n/2n − 1 for the n-th energy level. The Dirac equation relativistic spectrum is, however, easily recovered if the orbital momentum quantum number is replaced by total angular momentum quantum number j. In January 1926, Schrödinger submitted for publication instead his equation, a non-relativistic approximation that predicts the Bohr energy levels of hydrogen without fine structure.

In 1926, soon after the Schrödinger equation was introduced, Vladimir Fock wrote an article about its generalization for the case of magnetic fields, where forces were dependent on velocity, and independently derived this equation. Both Klein and Fock used Kaluza and Klein’s method. Fock also determined the gauge theory for the wave equation. The Klein–Gordon equation for a free particle has a simple plane wave solution.

The non-relativistic equation for the energy of a free particle is

By quantizing this, we get the non-relativistic Schrödinger equation for a free particle,

where

is the momentum operator ( being the del operator), and

is the energy operator.

The Schrödinger equation suffers from not being relativistically invariant, meaning that it is inconsistent with special relativity.

It is natural to try to use the identity from special relativity describing the energy:

Then, just inserting the quantum mechanical operators for momentum and energy yields the equation

The square root of a differential operator can be defined with the help of Fourier transformations, but due to the asymmetry of space and time derivatives, Dirac found it impossible to include external electromagnetic fields in a relativistically invariant way. So he looked for another equation that can be modified in order to describe the action of electromagnetic forces. In addition, this equation, as it stands, is nonlocal (see also ).

Klein and Gordon instead began with the square of the above identity, i.e.

which, when quantized, gives

which simplifies to

Rearranging terms yields

Since all reference to imaginary numbers has been eliminated from this equation, it can be applied to fields that are real valued as well as those that have complex values.

Rewriting the first two terms using the inverse of the Minkowski metric diag(−c2, 1, 1, 1), and writing the Einstein summation convention explicitly we get

Thus the Klein–Gordon equation can be written in a covariant notation. This often means an abbreviation in the form of

where

and

This operator is called the d’Alembert operator.

Today this form is interpreted as the relativistic field equation for spin-0 particles. Furthermore, any component of any solution to the free Dirac equation (for a spin-one-half particle) is automatically a solution to the free Klein–Gordon equation[why?]. This generalizes to particles of any spin due extension to the Bargmann–Wigner equations. Furthermore, in quantum field theory, every component of every quantum field must satisfy the free Klein–Gordon equation, making the equation a generic expression of quantum fields.

The Klein–Gordon equation can be generalized to describe a field in some potential V(ψ) as:

The conserved current associated to the U(1) symmetry of a complex field





ϕ



(


x


)







C





{\displaystyle \phi (x)\in \mathbb {C} }


satisfying the Klein–Gordon equation reads

The form of the conserved current can be derived systematically by applying Noether’s theorem to the U(1) symmetry. We will not do so here, but simply give a proof that this conserved current is correct.

From the Klein Gordon equation for a complex field





ϕ



(


x


)




{\displaystyle \phi (x)}


of mass





m




{\displaystyle m}


written in covariant notation

and its complex conjugate

we have, multiplying by the left respectively by






ϕ










(


x


)




{\displaystyle \phi ^{*}(x)}


and





ϕ



(


x


)




{\displaystyle \phi (x)}


(and omitting for brevity the explicit




x




{\displaystyle x}


dependence),

Subtracting the former from the latter we obtain

from which we obtain the conservation law for the Klein Gordon field:

The Klein–Gordon equation for a free particle can be written as

We look for plane wave solutions of the form

for some constant angular frequency ω ∈ ℝ and wave number k ∈ ℝ3. Substitution gives the dispersion relation:

Energy and momentum are seen to be proportional to ω and k:

So the dispersion relation is just the classic relativistic equation:

For massless particles best stainless steel water bottle, we may set m = 0, recovering the relationship between energy and momentum for massless particles:

The Klein–Gordon equation can also be derived via a variational method by considering the action:

where ψ is the Klein–Gordon field and m is its mass. The complex conjugate of ψ is written ψ. If the scalar field is taken to be real-valued, then ψ = ψ.

Applying the formula for the Hilbert stress–energy tensor to the Lagrangian density (the quantity inside the integral), we can derive the stress–energy tensor of the scalar field. It is

By integration of the time–time component T00 over all space, one may show that both the positive and negative frequency plane wave solutions can be physically associated with particles with positive energy. This is not the case for the Dirac equation and its energy–momentum tensor.

There is a simple way to make any field interact with electromagnetism in a gauge invariant way: replace the derivative operators with the gauge covariant derivative operators. This is because to maintain symmetry of the physical equations for the wavefunction





ϕ





{\displaystyle \phi }


under a local U(1) gauge transformation





ϕ








ϕ







=


e


x


p


(


i


θ



)


ϕ





{\displaystyle \phi \rightarrow \phi ‘=exp(i\theta )\phi }


where





θ



(


t


,




x




)




{\displaystyle \theta (t,{\textbf {x}})}


is a locally variable phase angle, which transformation redirects the wavefunction in the complex phase space defined by





e


x


p


(


i


θ



)


=


c


o


s


θ



+


i


s


i


n


θ





{\displaystyle exp(i\theta )=cos\theta +isin\theta }


, it is required that ordinary derivatives











μ







{\displaystyle \partial _{\mu }}







D



μ





=








μ









i


e



A



μ







{\displaystyle D_{\mu }=\partial _{\mu }-ieA_{\mu }}


while the gauge fields transform as





e



A



μ









e



A



μ








=


e



A



μ





+








μ





θ





{\displaystyle eA_{\mu }\rightarrow eA’_{\mu }=eA_{\mu }+\partial _{\mu }\theta }


. The Klein Gordon equation therefore becomes:

in natural units, where A is the vector potential. While it is possible to add many higher order terms, for example,

these terms are not renormalizable in 3+1 dimensions.

The field equation for a charged scalar field multiplies by i,[clarification needed] which means the field must be complex. In order for a field to be charged, it must have two components that can rotate into each other, the real and imaginary parts.

The action for a charged scalar is the covariant version of the uncharged action:

In general relativity, we include the effect of gravity by replacing partial with covariant derivatives and the Klein–Gordon equation becomes (in the mostly pluses signature)

or equivalently

where gαβ is the inverse of the metric tensor that is the gravitational potential field, g is the determinant of the metric tensor, μ is the covariant derivative and Γσμν is the Christoffel symbol that is the gravitational force field.

Banan

September 13th, 2017

En banan er det aflange bær, som bæres af bananplanten. I daglig tale betegnes bananen som frugt metal water bottle safety, men botanisk set er der tale om et bær. Frugten er blandt de mest spiste i verden og spises både som rå frugt og tilberedt i bl.a. desserter som bananasplit, banoffee pie og bananroulade

Bananfrugten inddeles i fire forskellige sorter. Den almindeligt kendte gule banan tilhører sorten melbanan. Endvidere findes den i en grøn variant, som er sorten æblebanan

Lady’s finger er kendetegnet ved dens ret korte længde i forhold til de andre sorter football shirt customizer. Dens længde er typisk på størrelse med en finger – heraf navnet, der betyder kvindes finger. På tysk kendes den også som babybanan. Denne findes også som en rød variant.

Alle bananerne har en tynd skal, så det er nemt at skrælle den.

Bananer indeholder ca. 74 % vand shaver outlet, 23 % kulhydrater, 1 % proteiner, 0,5 % fedt og 2,6 % fibre alt efter modenhed og vækstbetingelser. I en umoden banan er kulhydraterne mest stivelse thermos flask price. I modningsprocessen bliver stivelsen omdannet til sukker; en fuldmoden banan har kun 1–2 % stivelse. Højt sukkerindhold betyder, at bananen har et højere energiindhold end æbler eller appelsiner.

Den mest populære banantype, Cavendish, reproducerer sig ikke kønsligt og har derfor ingen variation i arveanlæggene. Det gør planten meget udsat for specifikke sygdomme, der i værste fald på én gang kan udrydde alle ens planter.

Konventionelt dyrkede bananer sprøjtes normalt med svampegift for at undgå sygdomsangreb. En af sygdommene er Black Sigatoka, der skyldes svampen med navnet mycosphaerella fijiensis (først beskrevet i 1964).

Toronto Blue Ice Jets

September 13th, 2017

The Toronto Blue Ice Jets were a Canadian Junior ice hockey team based out of Thornhill, Ontario, Canada. The team played in the Greater Metro Junior A Hockey League (GMHL).

The Jets were Thornhill’s only Junior hockey team after the Ontario Provincial Junior A Hockey League’s Toronto Thunderbirds relocated to King City to become the Villanova Knights.

They were founded as the Toronto Canada Moose in the inaugural year of the GMHL in the 2006–07 season as one of seven original league members. The first game took place on September 9, 2006, against the King Wild in Thornhill, Ontario resulting in a 5-1 loss. On September 11 sock cleats, 2006, the team earned their first win defeating the Deseronto Thunder by a score of 5-2. The Moose finished their inaugural season with a 19-20-0-3 record. They placed fifth in the league after a season long race for fourth with the Deseronto Thunder and Nipissing Alouettes. Their first playoff appearance put them up against the King Wild in the league quarterfinals. Unfortunately, the Moose were eliminated in five games in a best-of-seven series (3-8, 8-3, 3-5, 1-9, 2-6) remington fabric shaver.

The Moose started their second season off very slowly. After breaking a long losing streak, the Moose managed to earn fourteen more wins but still only finished in eleventh place in the now thirteen team league. In the first round, the Moose were picked to oppose the top seeded Bradford Rattlers. The Moose managed to keep it close over the first three games but the Rattlers still swept the series in four games.

On January 3, 2008, the Moose played against Kazakhstan’s Torpedo UST-Kamenogorsk Under-18 squad in an exhibition game. Despite rallying to tie the game 4-4 at the end of the second, the Moose fell to the Torpedo 8-5.

In spring 2013, the Moose were renamed the Blue Ice Jets. On September 6, 2013, the Blue Ice Jets played their first game since changing ownership against South Muskoka Shield and lost 5-4. The first win under the Blue Ice Jets name took place on September 7, 2013 against the Bobcaygeon Bucks in Thornhill, Ontario. The Blue Ice Jets beat the Bucks 17-2.

For the 2016–17 season, the Blue Ice Jets were scheduled to play their first home game on September 6, 2016. However, the team never took the ice and within a week the Blue Ice Jets had been removed from the GMHL. On September 13, the GMHL president stated that the Blue Ice Jets had taken the season off and possibly plans to relocate for the next season.

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