ACONDICIONAMIENTO DE SEÑAL - Departament de...

3
1 ACONDICIONAMIENTO DE SEÑAL Potenciómetro v m /V versus α=1-x El parámetro es K=R m /R n Error relativo ε= [v m -v m (R m =∞)]/ v m (R m =∞) versus x El parámetro es K=R m /R n

Transcript of ACONDICIONAMIENTO DE SEÑAL - Departament de...

Page 1: ACONDICIONAMIENTO DE SEÑAL - Departament de Físicadfs.uib.es/GTE/staff/jfont/InstrETT/condres1.pdf · Error absoluto a fondo de escala e= [v m-v m (R m = ∞)]/V versus 1-x ...

1

ACONDICIONAMIENTO DE SEÑAL

Potenciómetro

vm/V versus α=1-xEl parámetro es K=Rm/Rn

Error relativo ε= [vm-vm (Rm=∞)]/ vm (Rm=∞) versus xEl parámetro es K=Rm/Rn

Page 2: ACONDICIONAMIENTO DE SEÑAL - Departament de Físicadfs.uib.es/GTE/staff/jfont/InstrETT/condres1.pdf · Error absoluto a fondo de escala e= [v m-v m (R m = ∞)]/V versus 1-x ...

2

Error absoluto a fondo de escala e= [vm-vm (Rm=∞)]/V versus 1-xEl parámetro es K=Rm/Rn

Error absoluto a fondo de escala e= [vm-vm (Rm=∞)]/V versus 1-x (curva z) en caso dedos resistencias en paralelo Rm y vm (x=1/2)=vm (Rm=∞)La curva y corresponde a la anterior gráficaLa curva s corresponde si se usa alimentación simétricaEl parámetro es K=Rm/Rn=10 para los tres casos

Page 3: ACONDICIONAMIENTO DE SEÑAL - Departament de Físicadfs.uib.es/GTE/staff/jfont/InstrETT/condres1.pdf · Error absoluto a fondo de escala e= [v m-v m (R m = ∞)]/V versus 1-x ...

3

Linealización de un termistor con un divisor de tensión

F(T)=1/(1+ s exp (B(1/T-1/To))) versus T(ºC)El parámetro es s = Ro/R


Patterson Space, Molecular Replacement and Heavy Atom ...Symmetry positions are calculated using symops (M, v) x’ = Mx + v (M is the matrix and v is the vector) Combining, we can

Patterson Space, Molecular Replacement and Heavy Atom ...Symmetry positions are calculated using symops (M, v) x’ = Mx + v (M is the matrix and v is the vector) Combining, we can

V(r) r rmrm εmεm r=σ Regione attrattiva Regione repulsiva V(r m )=-ε, F attr =F rep V(σ)=0, V attr =V rep.

V(r) r rmrm εmεm r=σ Regione attrattiva Regione repulsiva V(r m )=-ε, F attr =F rep V(σ)=0, V attr =V rep.

21. Integral momentum equation · Moment-of-momentum equation () s V A V A r v dV r v vdA r gdV r pdA M M t ×ρ + × ρ = ×ρ − × − + ∂ ∂ ∫ ∫ ∫ ∫ 22. Application

21. Integral momentum equation · Moment-of-momentum equation () s V A V A r v dV r v vdA r gdV r pdA M M t ×ρ + × ρ = ×ρ − × − + ∂ ∂ ∫ ∫ ∫ ∫ 22. Application

3 . * / # ( $ % * / - / - . ' . * - · % 0 & $ * 4 o e o m s ã % ` o g m q r m s 5 o @ m s k = e z r m s p = o v [ - r m g v b \ = b n g h m g k x k \ = q t ä u t m p m k b v m

3 . * / # ( $ % * / - / - . ' . * - · % 0 & $ * 4 o e o m s ã % ` o g m q r m s 5 o @ m s k = e z r m s p = o v [ - r m g v b \ = b n g h m g k x k \ = q t ä u t m p m k b v m

9.2 The Sinusoidal Response it() Ω 201/Chapter 9.pdf · m. cos( )ωφ {} jt V e m = ℜ . ωφ+ {} jt j. V ee m = ℜ. ωφ {} j jt. v Ve e m =ℜ. φω. j. Ve m {} cos( ) = φ P.

9.2 The Sinusoidal Response it() Ω 201/Chapter 9.pdf · m. cos( )ωφ {} jt V e m = ℜ . ωφ+ {} jt j. V ee m = ℜ. ωφ {} j jt. v Ve e m =ℜ. φω. j. Ve m {} cos( ) = φ P.

Mët t i l»u ngn gån v· Lþ thuy¸t Ph¤m trò v H m tû · Mët t i l»u ngn gån v· Lþ thuy¸t Ph¤m trò v H m tû A short way to Theory of Categories and Functors Author:

Mët t i l»u ngn gån v· Lþ thuy¸t Ph¤m trò v H m tû · Mët t i l»u ngn gån v· Lþ thuy¸t Ph¤m trò v H m tû A short way to Theory of Categories and Functors Author:

SPR-54 : LEDs · spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m)

SPR-54 : LEDs · spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m) spr-54mvw(v) spr-54mvw(m)

[][]A α B - Universitat Jaume Irajadell/index_files/IA14/tema12.pdf2 [] [][] [][]m n d i A d i k A B k M N dt 1 d A v v v = − ν = − = α β (12.1) En el equilibrio se igualan

[][]A α B - Universitat Jaume Irajadell/index_files/IA14/tema12.pdf2 [] [][] [][]m n d i A d i k A B k M N dt 1 d A v v v = − ν = − = α β (12.1) En el equilibrio se igualan

V… ¥…EÚ…∫… - marwarisammelan.commarwarisammelan.com/admin/uploads/magazine/Samaj_bikash_August... · ∫………V… ¥…EÚ…∫…, +M…∫i… 2017 3 ∫………V…

V… ¥…EÚ…∫… - marwarisammelan.commarwarisammelan.com/admin/uploads/magazine/Samaj_bikash_August... · ∫………V… ¥…EÚ…∫…, +M…∫i… 2017 3 ∫………V…

MOMENTUM. DEFINITIONS Linear momentum (p) is defined as the product of mass (m) and velocity (v): p = m x v SI-unit of momentum is 1 kg ∙ m ∙ s -1, alternative.

MOMENTUM. DEFINITIONS Linear momentum (p) is defined as the product of mass (m) and velocity (v): p = m x v SI-unit of momentum is 1 kg ∙ m ∙ s -1, alternative.

THE NEGATIVE-FEEDBACK LOOP - College of Engineering ... · I V ICVS 0 0 i to v v o/i i r m Trans-resistance amplifier V I VCIS ¥ ¥ v to ... Stability of the negative feedback loop

THE NEGATIVE-FEEDBACK LOOP - College of Engineering ... · I V ICVS 0 0 i to v v o/i i r m Trans-resistance amplifier V I VCIS ¥ ¥ v to ... Stability of the negative feedback loop

Lizio, M. G., Andrushchenko, V ... - University of Bristol

Lizio, M. G., Andrushchenko, V ... - University of Bristol

TIPOS PSICOLÓGICOS - Creaciones Imaginales · gridad aproximada, sobrepasaría con mucho mis fuerzas, resultaría además que no contribuiría fun-damentalmente, en absoluto, a enriquecer

TIPOS PSICOLÓGICOS - Creaciones Imaginales · gridad aproximada, sobrepasaría con mucho mis fuerzas, resultaría además que no contribuiría fun-damentalmente, en absoluto, a enriquecer

Position-Time Graphs. POSITION (m) TIME (s) 10 20 30 40 50 5 10 1520 25 0 0 v = v = 2 m/s [E] 50 - 30 25 - 15 v = Δd Δt v = 35 - 15 17.5 - 7.5.

Position-Time Graphs. POSITION (m) TIME (s) 10 20 30 40 50 5 10 1520 25 0 0 v = v = 2 m/s [E] 50 - 30 25 - 15 v = Δd Δt v = 35 - 15 17.5 - 7.5.

YUTAKI M SERIES RASM-(3-6)(V)NE - Domotelec

YUTAKI M SERIES RASM-(3-6)(V)NE - Domotelec

1.1 INTRODUCTION 1.2 … · POROSITÉS 3 as = [1.4] M s V t = M s V s +V v ρas =massevolumiqueapparentesèchedu sol (g/cm3) La masse volumique apparente sèche d’un sol est toujours

1.1 INTRODUCTION 1.2 … · POROSITÉS 3 as = [1.4] M s V t = M s V s +V v ρas =massevolumiqueapparentesèchedu sol (g/cm3) La masse volumique apparente sèche d’un sol est toujours

AstrofisicaNucleare Chiodini StrutturaStellare...ρ=M/V dρ=-MdV V2 =-ρdV V Lavoro M = Scritto in termini di ρ e p 3. Energia di origine nucleare prodotta dalla massa unitaria nell’unità

AstrofisicaNucleare Chiodini StrutturaStellare...ρ=M/V dρ=-MdV V2 =-ρdV V Lavoro M = Scritto in termini di ρ e p 3. Energia di origine nucleare prodotta dalla massa unitaria nell’unità

Niels Bohr and the dawn of quantum theory - Weinberger · 3074 P. Weinberger v = V M M +m 2sinϑ, [where] 2ϑ is the angle through which the direction of the relative motion is deflected

Niels Bohr and the dawn of quantum theory - Weinberger · 3074 P. Weinberger v = V M M +m 2sinϑ, [where] 2ϑ is the angle through which the direction of the relative motion is deflected

PER TTE - prof6ghetti.weebly.com · d a tà o tà ε− σ v ʹ e − σ v ʹ a v = Δe / Δ(σ v ʹ ) ed v v E m m /1 / ( ) = = Δε Δ σʹ ... p d p E d = α⋅ q c E d = α⋅

PER TTE - prof6ghetti.weebly.com · d a tà o tà ε− σ v ʹ e − σ v ʹ a v = Δe / Δ(σ v ʹ ) ed v v E m m /1 / ( ) = = Δε Δ σʹ ... p d p E d = α⋅ q c E d = α⋅

DesarrollodeTeoremasparalaIntegralde Riemann ... · de f,α,a,b y en lo absoluto del símbolo x que puede ser remplazado por cualquierotrosinqueafecteparanadalaintegral. 3.1. PropiedadesLineales

DesarrollodeTeoremasparalaIntegralde Riemann ... · de f,α,a,b y en lo absoluto del símbolo x que puede ser remplazado por cualquierotrosinqueafecteparanadalaintegral. 3.1. PropiedadesLineales