R ( ) - studentski.netstudentski.net/get/ulj_fel_el1_mer_sno_mostici__formule_01.pdfMaxwellov...

1
Wheatstonov mostič: ( 29 + + + + + + ∆ = ∆ = 10 2 2 10 5 4 3 2 10 0 5 10 1 2 R R R R R R R R R U I R R q q δ 10 2 mR R = 10 3 nR R = 10 4 mnR R = 10 5 pR R = ( 29 ( 29 [ ] m m p mn n m R U I q q + + + + + + ∆ = - 2 1 1 10 0 5 δ Thomsonov (Kelvinov) mostič: ( 29 + + ∆ = 4 3 3 10 0 5 1 2 R R R R R I I g q q δ Izmenični mostiči: ( 29 + + ∆ = 10 2 2 10 0 5 2 Z Z Z Z U U q q δ Wheatstonov mostič: Splošno: 3 2 4 1 Z Z Z Z = 3 2 4 1 ϕ ϕ ϕ ϕ + = + Induktivni: L L U U V ∆ = 0 2 1 Ownov mostič: + = + 2 2 4 3 1 1 1 C j R Z Z L j R ϖ ϖ 3 3 4 3 C R j Z Z ϖ = Maxwellov mostič: ( 29 3 3 4 2 1 1 L j R Z Z L j R ϖ ϖ + = + 4 2 4 2 R R Z Z = Maxwell-Wienov mostič: + = + 4 4 3 2 1 1 1 C j R Z Z L j R ϖ ϖ 3 2 3 2 R R Z Z =

Transcript of R ( ) - studentski.netstudentski.net/get/ulj_fel_el1_mer_sno_mostici__formule_01.pdfMaxwellov...

Page 1: R ( ) - studentski.netstudentski.net/get/ulj_fel_el1_mer_sno_mostici__formule_01.pdfMaxwellov mostič: (3 3) 4 2 1 1 R j L Z Z R +j ...

Wheatstonov mostič:

( )

++++++

∆=

∆=

10

2

2

10543210

0

5

10

1 2R

R

R

RRRRRR

U

I

R

R qqδ

102 mRR = 103 nRR = 104 mnRR = 105 pRR =( ) ( )[ ]mmpmnnmRU

I qq ++++++

∆= − 21 1

100

5δ

Thomsonov (Kelvinov) mostič:

( )

++

∆=

4

33

100

512

R

RRR

RI

Ig

qqδ

Izmenični mostiči:( )

++

∆=

10

2

2

10

0

52

Z

Z

Z

Z

U

U qqδ

Wheatstonov mostič: Splošno: 3241 ZZZZ = 3241 ϕϕϕϕ +=+

Induktivni: L

LUUV

∆= 02

1

Ownov mostič:

+=+

22

4

311

1

CjR

Z

ZLjR

ωω 33

4

3 CRjZ

Z ω=

Maxwellov mostič: ( )334

211 LjR

Z

ZLjR ωω +=+

4

2

4

2

R

R

Z

Z =

Maxwell-Wienov mostič:

+=+ 4

43211

1Cj

RZZLjR ωω 3232 RRZZ =

Interaction of Charged Particles with Matter · dr r Z dr r Z r d rr e r Vr edr r r e eZ ... eigen functions. W. Udo Schröder, 2009 Nuclear Deformations 6. Restrictions on Nuclear

Interaction of Charged Particles with Matter · dr r Z dr r Z r d rr e r Vr edr r r e eZ ... eigen functions. W. Udo Schröder, 2009 Nuclear Deformations 6. Restrictions on Nuclear

Splošno o DSP 1 - studentski.netstudentski.net/get/ulj_fel_el2_dp2_sno_splosno_o_dsp_01.pdf · Diskretna Fourierjeva transformacija ∑ − = = − 1 0 ( ) ( )exp[ (2 / )] N n X

Splošno o DSP 1 - studentski.netstudentski.net/get/ulj_fel_el2_dp2_sno_splosno_o_dsp_01.pdf · Diskretna Fourierjeva transformacija ∑ − = = − 1 0 ( ) ( )exp[ (2 / )] N n X

: Variáveis padronizadas Z t = ( Z (1) Z (1) (2) Z(1) Z(2) Z · YX Y, X Y V Corr ( ) ... Proporção de variação explicada Considere a retenção de r variáveis canônicas, então,

: Variáveis padronizadas Z t = ( Z (1) Z (1) (2) Z(1) Z(2) Z · YX Y, X Y V Corr ( ) ... Proporção de variação explicada Considere a retenção de r variáveis canônicas, então,

Phase Transformations and Mechanical d r ñ õ ì £ í Z tY v ...

Phase Transformations and Mechanical d r ñ õ ì £ í Z tY v ...

Problema A.2. Setembre 2012...Ricard Peiró i Estruch 1 Problema A.2. Setembre 2012 En l’espai es té la recta r i el pla Π d’equacions − − = + − = ≡ x y z 0 x y z 1 r

Problema A.2. Setembre 2012...Ricard Peiró i Estruch 1 Problema A.2. Setembre 2012 En l’espai es té la recta r i el pla Π d’equacions − − = + − = ≡ x y z 0 x y z 1 r

Flore Skaza CEA-Saclay/DSM/DAPNIA/SPhN. Z Z N 2468 10 2 4 Be Li He H 8 He r = r 0 A 1/3 (r 0 = 1.2 fm) 208 Pb 11 Li = 9 Li + 2n 6 He 4 He 3 He 11 Li.

Flore Skaza CEA-Saclay/DSM/DAPNIA/SPhN. Z Z N 2468 10 2 4 Be Li He H 8 He r = r 0 A 1/3 (r 0 = 1.2 fm) 208 Pb 11 Li = 9 Li + 2n 6 He 4 He 3 He 11 Li.

N r G s · 2021. 1. 21. · G r r x s r ~t Z ( ] o Á ] Z } Á U 2 X 2 r 3 v U x X í ô9 ì. ^ : { s x s _ rs X s v' } P Z í ô ô ñ 4 { v r X X X G A { r v v x õ

N r G s · 2021. 1. 21. · G r r x s r ~t Z ( ] o Á ] Z } Á U 2 X 2 r 3 v U x X í ô9 ì. ^ : { s x s _ rs X s v' } P Z í ô ô ñ 4 { v r X X X G A { r v v x õ

Generalized Social Marginal Welfare Weights for Optimal Tax ......R i w iu ci dT(z i) = R i g idT(z i). ChangeintaxpaidperpersonisdT(z i)+T0(z i)dz i. Definition AreformdT(z) isbudgetneutralifandonlyif

Generalized Social Marginal Welfare Weights for Optimal Tax ......R i w iu ci dT(z i) = R i g idT(z i). ChangeintaxpaidperpersonisdT(z i)+T0(z i)dz i. Definition AreformdT(z) isbudgetneutralifandonlyif

A Computational Analysis of a Two-Fluid non-Linear ...e-jst.teiath.gr/issues/issue_42/Siddiqui_42.pdf · Fzz R or dG S ... N N u if R z r R z r WP w d d w (6) Where R p is the radius

A Computational Analysis of a Two-Fluid non-Linear ...e-jst.teiath.gr/issues/issue_42/Siddiqui_42.pdf · Fzz R or dG S ... N N u if R z r R z r WP w d d w (6) Where R p is the radius

Mechanics - hkage.org.hkhkage.org.hk/en/imo_pho/pho09/HKPHO_Booklet2.pdf1 Mechanics 1 Vector 1.1 Any vector x 0 y 0 z A A x A y A z 0 r r r r = + + (1.1) Addition of two vectors: x

Mechanics - hkage.org.hkhkage.org.hk/en/imo_pho/pho09/HKPHO_Booklet2.pdf1 Mechanics 1 Vector 1.1 Any vector x 0 y 0 z A A x A y A z 0 r r r r = + + (1.1) Addition of two vectors: x

ques_mains.pdf... · 2019-03-13 · 2 EMT 1. Two homogeneous isotropic dielectrics are separated by plane z = 0. For z > 0 ; ϵ r = 4 and E 3ax–4ay 6az kV/m If ϵ r = 3 for z

ques_mains.pdf... · 2019-03-13 · 2 EMT 1. Two homogeneous isotropic dielectrics are separated by plane z = 0. For z > 0 ; ϵ r = 4 and E 3ax–4ay 6az kV/m If ϵ r = 3 for z

A G O R A F O B I A Z U N B E L T Z

A G O R A F O B I A Z U N B E L T Z

o µ } } } } v t r ] l } v d Z u } u Á ] Z d u µ r v v u ... · P U í î X ì u u } o v u Z Ç o ï U ñ r ] r r µ Ç o v Ì } ~ í X ò ñ P U ò X ó u u } o Á } Z u ] Æ µ

o µ } } } } v t r ] l } v d Z u } u Á ] Z d u µ r v v u ... · P U í î X ì u u } o v u Z Ç o ï U ñ r ] r r µ Ç o v Ì } ~ í X ò ñ P U ò X ó u u } o Á } Z u ] Æ µ

R E C E N Z I I

R E C E N Z I I

Rotação de Corpos Rígidos (Cap. 9) - Moodle USP: e ... · Analogia TranslaçãoRotação R θ m x y m R z z F r a d F F t a n F z OBS: Corpo Rígido Forças de vínculo compensam

Rotação de Corpos Rígidos (Cap. 9) - Moodle USP: e ... · Analogia TranslaçãoRotação R θ m x y m R z z F r a d F F t a n F z OBS: Corpo Rígido Forças de vínculo compensam

Policy Gradient Algorithms - Stanford · 2020. 9. 20. · Policy Gradient Theorem (PGT) Theorem r J( ) = Z S ˆˇ(s) Z A r ˇ(s;a; ) Qˇ(s;a) da ds Note: ˆˇ(s) depends on , but

Policy Gradient Algorithms - Stanford · 2020. 9. 20. · Policy Gradient Theorem (PGT) Theorem r J( ) = Z S ˆˇ(s) Z A r ˇ(s;a; ) Qˇ(s;a) da ds Note: ˆˇ(s) depends on , but

6. Laminar and turbulent boundary layers · net heat conductionrate out of R + Z R qdR_ | {z } rate of heat generationinR (6.36) Foraconstantpressureflowfield. ... Heattransfer-Convection

6. Laminar and turbulent boundary layers · net heat conductionrate out of R + Z R qdR_ | {z } rate of heat generationinR (6.36) Foraconstantpressureflowfield. ... Heattransfer-Convection

Kursusnoter til BasisMatbasismat.compute.dtu.dk/basismat/basismatnoter.pdf · Kursusnoter til BasisMat Peter Beelen Søren Thomsen Peter Nørtoft Morten Brøns jzj=r z=reia arg(z)=a

Kursusnoter til BasisMatbasismat.compute.dtu.dk/basismat/basismatnoter.pdf · Kursusnoter til BasisMat Peter Beelen Søren Thomsen Peter Nørtoft Morten Brøns jzj=r z=reia arg(z)=a

PoorClusterCatalog Table 2. · Table 2. (continued) Name Coordinates N gal σ 46 Fate z N z Note Zwicky Cluster R Z f Z Abell CfA HCG Yerkes B1950 arcmin (1) (2) (3) (4) (5) (6) (7)

PoorClusterCatalog Table 2. · Table 2. (continued) Name Coordinates N gal σ 46 Fate z N z Note Zwicky Cluster R Z f Z Abell CfA HCG Yerkes B1950 arcmin (1) (2) (3) (4) (5) (6) (7)

EX. Potential for uniformly charged thin ringocw.nctu.edu.tw/course/physics/physics2_lecturenotes/970320.pdf · EX. Potential for uniformly charged thin ring Q r z R dφ dQ V Z =(

EX. Potential for uniformly charged thin ringocw.nctu.edu.tw/course/physics/physics2_lecturenotes/970320.pdf · EX. Potential for uniformly charged thin ring Q r z R dφ dQ V Z =(