=
n
⋅
l
⋅
a
2
{\displaystyle ={\frac {n\cdot l\cdot a}{2}}}
=
l
2
tan
(
π
n
)
{\displaystyle ={{l} \over {2\,\tan \left({{\pi } \over {n}}\right)}}}
=
n
l
2
4
tan
(
π
n
)
{\displaystyle ={{n\,l^{2}} \over {4\,\tan \left({{\pi } \over {n}}\right)}}}
=
l
⋅
1
⋅
a
{\displaystyle ={{l}\cdot 1\cdot a}}
w
=
k
m
{\displaystyle w={\sqrt {\frac {k}{m}}}}
F
=
−
m
g
θ
=
−
m
g
(
x
L
)
{\displaystyle F=-mg\theta =-mg({\frac {x}{L}})}
F
=
−
m
g
θ
=
−
(
m
g
L
)
x
{\displaystyle F=-mg\theta =-({\frac {mg}{L}})x}
F
=
−
k
x
{\displaystyle F=-kx}
k
=
m
g
/
L
{\displaystyle k=mg/L}
w
=
k
m
=
m
g
/
L
m
=
g
L
{\displaystyle w={\sqrt {\frac {k}{m}}}={\sqrt {\frac {mg/L}{m}}}={\sqrt {\frac {g}{L}}}}
T
=
2
π
w
=
2
π
L
g
{\displaystyle T={\frac {2\pi }{w}}=2\pi {\sqrt {\frac {L}{g}}}}
T
=
m
m
/
s
2
=
s
2
=
s
{\displaystyle T={\sqrt {\frac {m}{m/s^{2}}}}={\sqrt {s^{2}}}=s}
dimentsionalki homogeneoa.
;
{\displaystyle ;}
kasu bereziak, g=0 eta L=infinitu
lim
g
→
0
T
=
2
π
L
g
=
∞
{\displaystyle \lim _{g\to 0}T=2\pi {\sqrt {\frac {L}{g}}}=\infty }
lim
L
→
∞
T
=
2
π
L
g
=
∞
{\displaystyle \lim _{L\to \infty }T=2\pi {\sqrt {\frac {L}{g}}}=\infty }
v
=
2
q
V
m
{\displaystyle v={\sqrt {\frac {2qV}{m}}}}
v
=
2
q
σ
d
ε
0
m
{\displaystyle v={\sqrt {\frac {2q\sigma d}{\varepsilon _{0}m}}}}
C
=
ε
0
ε
r
A
d
{\displaystyle C=\varepsilon _{0}\varepsilon _{r}{\frac {A}{d}}}
non C kondentsadorearen kapazitatea den,
ε
0
{\displaystyle \varepsilon _{0}}
hutsean permitibitatea (
F
m
{\displaystyle {\frac {F}{m}}}
(Faraday/metro) magnitudekoa),
ε
r
{\displaystyle \varepsilon _{r}}
konstante dielektrikoa, A plaka paralelo bakoitzaren azalera (bere magnitudea
m
2
{\displaystyle m^{2}}
metro karratu izanda) eta d plaka paraleloen arteko distantzia (bere magnitudea
m
{\displaystyle m}
metro izanda)
C
=
F
m
m
2
m
=
F
{\displaystyle C={\frac {F}{m}}{\frac {m^{2}}{m}}=F}
; beraz, dimentsionalki homogeneoa da.
F
m
a
g
=
q
⋅
v
→
⋅
B
→
=
q
⋅
V
⋅
B
⋅
S
i
n
90
{\displaystyle F_{mag}=q\cdot {\vec {v}}\cdot {\vec {B}}=q\cdot V\cdot B\cdot Sin90}
(1)
F
z
=
m
⋅
v
2
R
{\displaystyle F_{z}=m\cdot {\frac {v^{2}}{R}}}
(2)
(
1
)
=
(
2
)
=>
F
m
a
g
=
F
z
{\displaystyle (1)=(2)=>F_{mag}=F_{z}}
q
⋅
v
⋅
B
=
m
⋅
v
2
R
{\displaystyle q\cdot v\cdot B=m\cdot {\frac {v^{2}}{R}}}
R
=
m
⋅
v
q
⋅
B
{\displaystyle R={\frac {m\cdot v}{q\cdot B}}}
R
=
k
g
⋅
m
s
C
⋅
T
=
k
g
⋅
m
s
C
k
g
C
⋅
s
=
k
g
⋅
C
⋅
s
⋅
m
s
⋅
C
⋅
k
g
=
m
{\displaystyle R={\frac {kg\cdot {\frac {m}{s}}}{C\cdot T}}={\frac {kg\cdot {\frac {m}{s}}}{C{\frac {kg}{C\cdot s}}}}={\frac {kg\cdot C\cdot s\cdot m}{s\cdot C\cdot kg}}=m}
Dimentsionalki homogeneoa da.a
a
a
a
a
[http//:www.a.com a]
Media:a.ogg
a
{\displaystyle a}
a
--Enzaiklopedia Nire eztabaida 13:08, 28 Otsaila 2008 (UTC)
--Enzaiklo
p
e
d
i
a
{\displaystyle pedia}
• Ezt ekarpenak 17:49, 9 Apirila 2008 (UTC)
En
z
a
i
{\displaystyle zai}
klo pe dia
a
{\displaystyle a}
a a a
a
{\displaystyle a}
a a a
£€ΒΘζΔδΞξΟΠρΣΦφΨΩ (keinuak)³²×~°
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Enzaiklopedia (eztabaida · ekarpenak )
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user-config.py Aldatu
family = 'wikipedia'
mylang = 'eu'
usernames['wikipedia']['eu'] = 'EnzaiBot'
usernames['wikipedia']['en'] = 'EnzaiBot'
usernames['wikipedia']['es'] = 'EnzaiBot'
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replace.py -ns:0 "Errror" "Error" -search:"Errror" -pt:1
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cosmetic_changes.py -start:! -always -pt:1
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Erreferentzin proba Aldatu
kaixo![2] sustatu, ez [3] ikusi testu errefenrentzi[4] ikus dezagun papayayo lanbide elektroniko albisteak[5]
ta orain referentziak jarri behian testu ahallokundiarra XD
[6]
Erreferentziak Aldatu
↑ Behekaldean agertzeko testua
↑ http://sustatu.net ikusi
↑ ratatoullie
↑ nada de esto fue un error, uoo, euskaraz mesedez
↑ Wikipedia:Albisteak
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