SlideShare a Scribd company logo
1 of 21
Transfer function model
 A standard second order transfer model
y(s) =ω02 /(s2 + 2ζωos + ω02)
Where,
ζ (zeta) is the relative damping factor
and ω0 [rad/s] is the undamped
resonance frequency.
Here in the charcteristic
equation
b=2ζωo
a=1(coefficient of s2 )
c= ω02
 Here the input is step input
Classification of second order
system
 First, if b = 0, the poles are complex
conjugates on the imaginary axis .This
corresponds to ζ = 0, and is referred to as the
undamped case.
 If b2 − 4ac < 0 then the poles are complex
conjugates lying in the left half of the s-
plane. This corresponds to the range 0 < ζ <
1, and is referred to as the underdamped
case.
If b2 − 4ac = 0 then the poles coincide
on the real axis at s1 = s2 = −b/2m. This
corresponds to ζ = 1, and is referred to
as the critically damped case.
Finally, if b2 − 4ac > 0 then the poles
are at distinct locations on the real axis
in the left half of the s-plane. This
corresponds to ζ > 1, and is referred to
as the overdamped case.
Undamped case (ζ = 0)
In this case, the poles lie at s1
= jωn and s2 = −jωn. The
homogeneous solution takes
the form
 x(t) = 1-cosωn t
Critically-damped ζ =1
In the critically damped case, ζ =1
and the two poles coincide at s =
−ωn. The response is then given
by :-
x(t)=1-e−ωnt –ωn (te−ωnt )(t ≥ 0).
Over damped ζ ≥1
One extremely important thing
to notice is that in this case the
roots are both negative.The
term under the square root is
positive by assumption, so the
roots are real.
General solution:
x(t) = 1-(0.5ωn /(ζ
2-1)
c1er’t + c2er’’t .
Under damped case (0 < ζ < 1)
The basic real solutions are:-
e−bt/2a cos(ωdt) and
e−bt/2a sin(ωdt).
 The general real solution is found by
taking linear combinations of the two
basic solutions, that is:
x(t) = 1-c1 ejωntcos(ωdt) - c2ejωntsin(ωdt)
where,
ωd = ωn(1−ζ2)1/2
is the damped natural frequency
Transient
Response (Under damped )
 Rise time
 The rise time, tr, is usually specified as the time
required for the output of the system to rise from
either 10% to 90%, 5% to 95%, or 0% to 100% of its
final value.
ωdtr + φ = π
Solving yields,
tr=(π –φ)/ ωd
Peak time
 Peak time, tp, is the time required for the output of the
system to reach its first peak. It is found by setting the
derivative of the output equal to zero.
tp =π /ωd
Settling Time
 Settling time, ts, is the time required for the output of
the system to reach and stay within a desired
percentage of the final value. Typically 2% or 5% is
used. The settling time is given by equation
ts = −ln(ǫ) /ζωn
where ǫ is the tolerance for 2% ǫ = 0.02, for 5% ǫ = 0.05,
etc
Maximum Percent OverShoot
 The maximum percent overshoot, Mp, is the peak
value of the output of the system divided by the final
value of the output. Substituting tp into the output,
equation will produce
Mp = e−ζπ /(√1−ζ2 )
Thank
you

More Related Content

What's hot

periodic functions and Fourier series
periodic functions and Fourier seriesperiodic functions and Fourier series
periodic functions and Fourier series
Umang Gupta
 
De Bruijn Superwalk with Multiplicities Problem is NP-hard
De Bruijn Superwalk with Multiplicities Problem is NP-hardDe Bruijn Superwalk with Multiplicities Problem is NP-hard
De Bruijn Superwalk with Multiplicities Problem is NP-hard
Alexey Sergushichev
 
On NP-Hardness of the Paired de Bruijn Sound Cycle Problem
On NP-Hardness of the Paired de Bruijn Sound Cycle ProblemOn NP-Hardness of the Paired de Bruijn Sound Cycle Problem
On NP-Hardness of the Paired de Bruijn Sound Cycle Problem
Fedor Tsarev
 

What's hot (20)

Termino n ésimo en una sucesion lineal y cuadratica
Termino n ésimo en una sucesion lineal y cuadraticaTermino n ésimo en una sucesion lineal y cuadratica
Termino n ésimo en una sucesion lineal y cuadratica
 
Fourier series
Fourier seriesFourier series
Fourier series
 
Sol71
Sol71Sol71
Sol71
 
To obtain steady state transient and sub transient short circuit currents of ...
To obtain steady state transient and sub transient short circuit currents of ...To obtain steady state transient and sub transient short circuit currents of ...
To obtain steady state transient and sub transient short circuit currents of ...
 
Laplace1
Laplace1Laplace1
Laplace1
 
periodic functions and Fourier series
periodic functions and Fourier seriesperiodic functions and Fourier series
periodic functions and Fourier series
 
Master method
Master methodMaster method
Master method
 
Fourier series 1
Fourier series 1Fourier series 1
Fourier series 1
 
Verlet's method
Verlet's methodVerlet's method
Verlet's method
 
GreedyAlgorithm
GreedyAlgorithmGreedyAlgorithm
GreedyAlgorithm
 
Laplace periodic function
Laplace periodic functionLaplace periodic function
Laplace periodic function
 
Fourier series and fourier integral
Fourier series and fourier integralFourier series and fourier integral
Fourier series and fourier integral
 
Nt lecture skm-iiit-bh
Nt lecture skm-iiit-bhNt lecture skm-iiit-bh
Nt lecture skm-iiit-bh
 
16100lectre14 cg
16100lectre14 cg16100lectre14 cg
16100lectre14 cg
 
Orthogonality relations pdf
Orthogonality relations pdfOrthogonality relations pdf
Orthogonality relations pdf
 
Markov Model for TMR System with Repair
Markov Model for TMR System with RepairMarkov Model for TMR System with Repair
Markov Model for TMR System with Repair
 
De Bruijn Superwalk with Multiplicities Problem is NP-hard
De Bruijn Superwalk with Multiplicities Problem is NP-hardDe Bruijn Superwalk with Multiplicities Problem is NP-hard
De Bruijn Superwalk with Multiplicities Problem is NP-hard
 
Spread spectrum communications and CDMA
Spread spectrum communications and CDMASpread spectrum communications and CDMA
Spread spectrum communications and CDMA
 
Probability
ProbabilityProbability
Probability
 
On NP-Hardness of the Paired de Bruijn Sound Cycle Problem
On NP-Hardness of the Paired de Bruijn Sound Cycle ProblemOn NP-Hardness of the Paired de Bruijn Sound Cycle Problem
On NP-Hardness of the Paired de Bruijn Sound Cycle Problem
 

Viewers also liked (13)

Second order systems
Second order systemsSecond order systems
Second order systems
 
42084837
4208483742084837
42084837
 
3Com 1.012.0743-B
3Com 1.012.0743-B3Com 1.012.0743-B
3Com 1.012.0743-B
 
3Com 3CP012884A
3Com 3CP012884A3Com 3CP012884A
3Com 3CP012884A
 
24346579
2434657924346579
24346579
 
Sehmahi ameen e shariyat feb. to apr.2017
Sehmahi ameen e shariyat feb. to apr.2017Sehmahi ameen e shariyat feb. to apr.2017
Sehmahi ameen e shariyat feb. to apr.2017
 
3Com 1667-310-050
3Com 1667-310-0503Com 1667-310-050
3Com 1667-310-050
 
Il caffè verde
Il caffè verdeIl caffè verde
Il caffè verde
 
Class 4 PowerPoint
Class 4 PowerPointClass 4 PowerPoint
Class 4 PowerPoint
 
Ad answers
Ad answersAd answers
Ad answers
 
Marca la diFErencia-ESO y Bachilerato
Marca la diFErencia-ESO y BachileratoMarca la diFErencia-ESO y Bachilerato
Marca la diFErencia-ESO y Bachilerato
 
Gpsppt 130412005659-phpapp01
Gpsppt 130412005659-phpapp01Gpsppt 130412005659-phpapp01
Gpsppt 130412005659-phpapp01
 
Redes sociales
Redes socialesRedes sociales
Redes sociales
 

Similar to Second order systems

Electrical Engineering - 2006 Unsolved Paper
Electrical Engineering - 2006 Unsolved PaperElectrical Engineering - 2006 Unsolved Paper
Electrical Engineering - 2006 Unsolved Paper
Vasista Vinuthan
 
tripple e 136 EMII2013_Chapter_10_P2.pdf
tripple e 136 EMII2013_Chapter_10_P2.pdftripple e 136 EMII2013_Chapter_10_P2.pdf
tripple e 136 EMII2013_Chapter_10_P2.pdf
AbdulgafforBaimpal1
 
Last+minute+revision(+Final)+(1) (1).pptx
Last+minute+revision(+Final)+(1) (1).pptxLast+minute+revision(+Final)+(1) (1).pptx
Last+minute+revision(+Final)+(1) (1).pptx
AryanMishra860130
 
L 11(gdr)(et) ((ee)nptel)
L 11(gdr)(et) ((ee)nptel)L 11(gdr)(et) ((ee)nptel)
L 11(gdr)(et) ((ee)nptel)
Pradeep Godara
 
TwoLevelMedium
TwoLevelMediumTwoLevelMedium
TwoLevelMedium
John Paul
 

Similar to Second order systems (20)

Time-Response Lecture
Time-Response LectureTime-Response Lecture
Time-Response Lecture
 
Crib Sheet AP Calculus AB and BC exams
Crib Sheet AP Calculus AB and BC examsCrib Sheet AP Calculus AB and BC exams
Crib Sheet AP Calculus AB and BC exams
 
Lect1
Lect1Lect1
Lect1
 
dynamical analysis of soil and structures
dynamical analysis of soil and structuresdynamical analysis of soil and structures
dynamical analysis of soil and structures
 
Mcrowave and Radar engineering
Mcrowave and Radar engineeringMcrowave and Radar engineering
Mcrowave and Radar engineering
 
Elementary Differential Equations 11th Edition Boyce Solutions Manual
Elementary Differential Equations 11th Edition Boyce Solutions ManualElementary Differential Equations 11th Edition Boyce Solutions Manual
Elementary Differential Equations 11th Edition Boyce Solutions Manual
 
Electrical Engineering - 2006 Unsolved Paper
Electrical Engineering - 2006 Unsolved PaperElectrical Engineering - 2006 Unsolved Paper
Electrical Engineering - 2006 Unsolved Paper
 
Berans qm overview
Berans qm overviewBerans qm overview
Berans qm overview
 
Antwoorden fourier and laplace transforms, manual solutions
Antwoorden   fourier and laplace transforms, manual solutionsAntwoorden   fourier and laplace transforms, manual solutions
Antwoorden fourier and laplace transforms, manual solutions
 
Solution a ph o 3
Solution a ph o 3Solution a ph o 3
Solution a ph o 3
 
tripple e 136 EMII2013_Chapter_10_P2.pdf
tripple e 136 EMII2013_Chapter_10_P2.pdftripple e 136 EMII2013_Chapter_10_P2.pdf
tripple e 136 EMII2013_Chapter_10_P2.pdf
 
Last+minute+revision(+Final)+(1) (1).pptx
Last+minute+revision(+Final)+(1) (1).pptxLast+minute+revision(+Final)+(1) (1).pptx
Last+minute+revision(+Final)+(1) (1).pptx
 
Microwave PPT.ppt
Microwave PPT.pptMicrowave PPT.ppt
Microwave PPT.ppt
 
L 11(gdr)(et) ((ee)nptel)
L 11(gdr)(et) ((ee)nptel)L 11(gdr)(et) ((ee)nptel)
L 11(gdr)(et) ((ee)nptel)
 
TwoLevelMedium
TwoLevelMediumTwoLevelMedium
TwoLevelMedium
 
First Order Active RC Sections
First Order Active RC SectionsFirst Order Active RC Sections
First Order Active RC Sections
 
Ch03 9
Ch03 9Ch03 9
Ch03 9
 
Pcv ch2
Pcv ch2Pcv ch2
Pcv ch2
 
2.1 Calculus 2.formulas.pdf.pdf
2.1 Calculus 2.formulas.pdf.pdf2.1 Calculus 2.formulas.pdf.pdf
2.1 Calculus 2.formulas.pdf.pdf
 
Laplace equation
Laplace equationLaplace equation
Laplace equation
 

Recently uploaded

Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort ServiceCall Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
9953056974 Low Rate Call Girls In Saket, Delhi NCR
 
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
9953056974 Low Rate Call Girls In Saket, Delhi NCR
 
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
ssuser89054b
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
dharasingh5698
 
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night StandCall Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
amitlee9823
 
AKTU Computer Networks notes --- Unit 3.pdf
AKTU Computer Networks notes ---  Unit 3.pdfAKTU Computer Networks notes ---  Unit 3.pdf
AKTU Computer Networks notes --- Unit 3.pdf
ankushspencer015
 

Recently uploaded (20)

Intze Overhead Water Tank Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank  Design by Working Stress - IS Method.pdfIntze Overhead Water Tank  Design by Working Stress - IS Method.pdf
Intze Overhead Water Tank Design by Working Stress - IS Method.pdf
 
Unleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leapUnleashing the Power of the SORA AI lastest leap
Unleashing the Power of the SORA AI lastest leap
 
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELLPVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
PVC VS. FIBERGLASS (FRP) GRAVITY SEWER - UNI BELL
 
Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort ServiceCall Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
Call Girls in Ramesh Nagar Delhi 💯 Call Us 🔝9953056974 🔝 Escort Service
 
Thermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.pptThermal Engineering -unit - III & IV.ppt
Thermal Engineering -unit - III & IV.ppt
 
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar  ≼🔝 Delhi door step de...
Call Now ≽ 9953056974 ≼🔝 Call Girls In New Ashok Nagar ≼🔝 Delhi door step de...
 
Online banking management system project.pdf
Online banking management system project.pdfOnline banking management system project.pdf
Online banking management system project.pdf
 
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
XXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXXX
 
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
(INDIRA) Call Girl Aurangabad Call Now 8617697112 Aurangabad Escorts 24x7
 
NFPA 5000 2024 standard .
NFPA 5000 2024 standard                                  .NFPA 5000 2024 standard                                  .
NFPA 5000 2024 standard .
 
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 BookingVIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
VIP Call Girls Ankleshwar 7001035870 Whatsapp Number, 24/07 Booking
 
chapter 5.pptx: drainage and irrigation engineering
chapter 5.pptx: drainage and irrigation engineeringchapter 5.pptx: drainage and irrigation engineering
chapter 5.pptx: drainage and irrigation engineering
 
Unit 1 - Soil Classification and Compaction.pdf
Unit 1 - Soil Classification and Compaction.pdfUnit 1 - Soil Classification and Compaction.pdf
Unit 1 - Soil Classification and Compaction.pdf
 
Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...Booking open Available Pune Call Girls Pargaon  6297143586 Call Hot Indian Gi...
Booking open Available Pune Call Girls Pargaon 6297143586 Call Hot Indian Gi...
 
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
The Most Attractive Pune Call Girls Manchar 8250192130 Will You Miss This Cha...
 
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night StandCall Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
Call Girls In Bangalore ☎ 7737669865 🥵 Book Your One night Stand
 
UNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its PerformanceUNIT - IV - Air Compressors and its Performance
UNIT - IV - Air Compressors and its Performance
 
Double rodded leveling 1 pdf activity 01
Double rodded leveling 1 pdf activity 01Double rodded leveling 1 pdf activity 01
Double rodded leveling 1 pdf activity 01
 
Water Industry Process Automation & Control Monthly - April 2024
Water Industry Process Automation & Control Monthly - April 2024Water Industry Process Automation & Control Monthly - April 2024
Water Industry Process Automation & Control Monthly - April 2024
 
AKTU Computer Networks notes --- Unit 3.pdf
AKTU Computer Networks notes ---  Unit 3.pdfAKTU Computer Networks notes ---  Unit 3.pdf
AKTU Computer Networks notes --- Unit 3.pdf
 

Second order systems

  • 1.
  • 2. Transfer function model  A standard second order transfer model y(s) =ω02 /(s2 + 2ζωos + ω02) Where, ζ (zeta) is the relative damping factor and ω0 [rad/s] is the undamped resonance frequency.
  • 3. Here in the charcteristic equation b=2ζωo a=1(coefficient of s2 ) c= ω02  Here the input is step input
  • 4. Classification of second order system  First, if b = 0, the poles are complex conjugates on the imaginary axis .This corresponds to ζ = 0, and is referred to as the undamped case.  If b2 − 4ac < 0 then the poles are complex conjugates lying in the left half of the s- plane. This corresponds to the range 0 < ζ < 1, and is referred to as the underdamped case.
  • 5. If b2 − 4ac = 0 then the poles coincide on the real axis at s1 = s2 = −b/2m. This corresponds to ζ = 1, and is referred to as the critically damped case. Finally, if b2 − 4ac > 0 then the poles are at distinct locations on the real axis in the left half of the s-plane. This corresponds to ζ > 1, and is referred to as the overdamped case.
  • 6. Undamped case (ζ = 0) In this case, the poles lie at s1 = jωn and s2 = −jωn. The homogeneous solution takes the form  x(t) = 1-cosωn t
  • 7.
  • 8. Critically-damped ζ =1 In the critically damped case, ζ =1 and the two poles coincide at s = −ωn. The response is then given by :- x(t)=1-e−ωnt –ωn (te−ωnt )(t ≥ 0).
  • 9.
  • 10. Over damped ζ ≥1 One extremely important thing to notice is that in this case the roots are both negative.The term under the square root is positive by assumption, so the roots are real.
  • 11. General solution: x(t) = 1-(0.5ωn /(ζ 2-1) c1er’t + c2er’’t .
  • 12.
  • 13. Under damped case (0 < ζ < 1) The basic real solutions are:- e−bt/2a cos(ωdt) and e−bt/2a sin(ωdt).
  • 14.  The general real solution is found by taking linear combinations of the two basic solutions, that is: x(t) = 1-c1 ejωntcos(ωdt) - c2ejωntsin(ωdt) where, ωd = ωn(1−ζ2)1/2 is the damped natural frequency
  • 15.
  • 16.
  • 17. Transient Response (Under damped )  Rise time  The rise time, tr, is usually specified as the time required for the output of the system to rise from either 10% to 90%, 5% to 95%, or 0% to 100% of its final value. ωdtr + φ = π Solving yields, tr=(π –φ)/ ωd
  • 18. Peak time  Peak time, tp, is the time required for the output of the system to reach its first peak. It is found by setting the derivative of the output equal to zero. tp =π /ωd
  • 19. Settling Time  Settling time, ts, is the time required for the output of the system to reach and stay within a desired percentage of the final value. Typically 2% or 5% is used. The settling time is given by equation ts = −ln(ǫ) /ζωn where ǫ is the tolerance for 2% ǫ = 0.02, for 5% ǫ = 0.05, etc
  • 20. Maximum Percent OverShoot  The maximum percent overshoot, Mp, is the peak value of the output of the system divided by the final value of the output. Substituting tp into the output, equation will produce Mp = e−ζπ /(√1−ζ2 )