SlideShare a Scribd company logo
2
Most read
5
Most read
6
Most read
INITIAL CONDITIONS : WHY TO STUDY
• Differential Equations written for a network
may contain arbitrary constants equal to the
order of the differential equations.
• The reason for studying initial conditions is to
find the value of arbitrary constants that
appear in the general solution of differential
equations written for a given network.
INITIAL CONDITIONS
• In Initial conditions, we find the change in selected variables
in a circuit when one or more switches are moved from open
to closed positions or vice versa.
t=0-
indicates the time just before changing
the position of the switch
t=0 indicates the time when the position of
switch is changed
t=0+
indicates the time immediately after
changing the position of switch
INITIAL CONDITIONS
• Initial condition focuses solely on the current
and voltages of energy storing elements
(inductor and capacitor) as they will
determine the circuit behavior at t>0.
• PAST HISTORY OF THE CIRCUIT WILL SHOW UP
AS THE CAPACITOR VOLTAGES AND INDUCTOR
CURRENTS
INITIAL CONDITIONS
1. RESISTOR
 The voltage current relation of an ideal resistance is
V=R*I
 From this equation it can be concluded that the
instantaneous current flowing through the resistor
changes if the instantaneous voltage across it
changes & vice versa
 The past voltage or current values have no effect on
the present or future working of the resistor i.e.. It’s
resistance remains the same irrespective of the past
conditions
INITIAL CONDITIONS
2. INDUCTOR
 The expression for current through the
inductor is given by
INITIAL CONDITIONS
Hence if i(0-
)=0A , then i(0+
)=0A
So we can visualize inductor as a open
circuit at t=0+
INITIAL CONDITIONS
• If i(0-
)=I0 , then i(0+
)=I0 i.e. the inductor can be
thought as a current source of I0 as shown
INITIAL CONDITIONS
FINAL CONDITIONS :
 From the basic relationship
V= L*(di/dt)
We can state that V=0 in steady state conditions at t= as
(di/dt)=0 due to constant current
INITIAL CONDITIONS
3. CAPACITOR
 The expression for voltage across the
capacitor is given by
INITIAL CONDITIONS
If V(0-
)=0V , then V(0+
)=0V indicating the
capacitor as a short circuit
INITIAL CONDITIONS
If V(0-
)= V volts, then the capacitor can be
visualized as a voltage source of V volts
INITIAL CONDITIONS
• Final Conditions
The current across the capacitor is given by the equation
i=C*(dv/dt)
which indicates that i=0A in steady state at t=
due to capacitor being fully charged.
INITIAL CONDITION
EXAMPLE-1 : In the network shown in the figure
the switch is closed at t=0. Determine i, (di/dt)
and (d2
i/dt2
) at t=0+
.
At t=0-
, the switch is
Closed. Due to which
il(0-
)=0A
Vc(0-
)=0V
INITIAL CONDITION
At t=0+
the circuit is
From the circuit
il(0+
)=0A
Vc(0+
)=0V
INITIAL CONDITION
• Writing KVL clockwise for the circuit
Putting t=0+
in equation (2)
INITIAL CONDITION
• Differentiating equation (1) with respect to time
INITIAL CONDITION
 Example 2: The position of switch was changed from
1 to 2 at t=0. Steady State was achieved when the
switch was at position 1. Find i, (di/dt) & (d2
i/dt2
) at
t=0+
INITIAL CONDITION
At t=0-
, the circuit is shown in figure
The inductor is in steady state so it is
assumed to be shorted.
So the current through it is
il(0-
)=20/10=2A
Vc(0-
)=0V
INITIAL CONDITION
So at t=0+
, the switch is at position 2
Here the Inductor behaves as a current source
of 2A. The circuit is shown below
il(0+
)=2A
Vc(0+
)=0V
INITIAL CONDITION
INITIAL CONDITION
THANK YOU

More Related Content

PDF
First order circuits linear circuit analysis
ZulqarnainEngineerin
 
PPT
dc circuits
Yasir Hashmi
 
PDF
DC Network - Comprehending Theorems
Aakash Yellapantulla
 
PDF
Millman's theorem
Syed Saeed
 
PPTX
BEEE-UNIT 1.pptx
Gigi203211
 
PPT
DC circuit
prempanigrahi
 
PPT
Delta star relationship (1)
140120109032
 
PPT
Electrical circuits dc network theorem
University of Potsdam
 
First order circuits linear circuit analysis
ZulqarnainEngineerin
 
dc circuits
Yasir Hashmi
 
DC Network - Comprehending Theorems
Aakash Yellapantulla
 
Millman's theorem
Syed Saeed
 
BEEE-UNIT 1.pptx
Gigi203211
 
DC circuit
prempanigrahi
 
Delta star relationship (1)
140120109032
 
Electrical circuits dc network theorem
University of Potsdam
 

What's hot (20)

PDF
Power electronics Phase Controlled Rectifiers - SCR
Burdwan University
 
PDF
Fault analysis
Revathi Subramaniam
 
PPT
Initial and final condition for circuit
vishalgohel12195
 
PPTX
Single phase full bridge inverter
Nisarg Amin
 
PPTX
Clipper and clamper circuits
Unsa Shakir
 
PPT
Over voltages in power system
SANGEETHA S
 
PPT
BUCK CONVERTER
NIT MEGHALAYA
 
PDF
Phase Controlled Rectifiers
maneesh001
 
PPTX
Classes of amplifiers
Arsalan Qureshi
 
PDF
Breaking,Types of Electrical Braking system, Regenerative Braking, Plugging ...
Waqas Afzal
 
PPTX
Single phase ac voltage controller
Swati Tiwari
 
PPTX
Three phase semi converter
Arpit Raval
 
PPTX
Skin effect, proximity effect, ferranti effect, corona discharge
RoungpaSukhe
 
PDF
Polar Plot
Hussain K
 
PDF
Gauss seidel method
Revathi Subramaniam
 
PPTX
TRIAC
Suresh Mohta
 
PDF
Power system stability
Balaram Das
 
PPTX
Power flow through transmission line.
SHI SAD VIDYA MANDAL INSTITUTE OF TECHNOLOGY
 
PDF
Thyristor
Burdwan University
 
PDF
Economic operation of power system
Balaram Das
 
Power electronics Phase Controlled Rectifiers - SCR
Burdwan University
 
Fault analysis
Revathi Subramaniam
 
Initial and final condition for circuit
vishalgohel12195
 
Single phase full bridge inverter
Nisarg Amin
 
Clipper and clamper circuits
Unsa Shakir
 
Over voltages in power system
SANGEETHA S
 
BUCK CONVERTER
NIT MEGHALAYA
 
Phase Controlled Rectifiers
maneesh001
 
Classes of amplifiers
Arsalan Qureshi
 
Breaking,Types of Electrical Braking system, Regenerative Braking, Plugging ...
Waqas Afzal
 
Single phase ac voltage controller
Swati Tiwari
 
Three phase semi converter
Arpit Raval
 
Skin effect, proximity effect, ferranti effect, corona discharge
RoungpaSukhe
 
Polar Plot
Hussain K
 
Gauss seidel method
Revathi Subramaniam
 
Power system stability
Balaram Das
 
Power flow through transmission line.
SHI SAD VIDYA MANDAL INSTITUTE OF TECHNOLOGY
 
Thyristor
Burdwan University
 
Economic operation of power system
Balaram Das
 
Ad

Similar to Initial Conditions of Resistor, Inductor & Capacitor (20)

PPT
Initial Conditions
Smit Shah
 
PPT
Initial Conditions
Soham Gajjar
 
PPTX
Initial condition
Ravi Patel
 
PDF
Lecture slides Ist & 2nd Order Circuits[282].pdf
sami717280
 
PDF
Second order circuits linear circuit analysis
ZulqarnainEngineerin
 
PPTX
RL RC _src - Basic electric theory .pptx
happycocoman
 
PDF
Assignmentl3 solutions
Om Prakash Bankolia
 
PPTX
Step respponse of rlc circuit by Aditya Pratap Singh Delhi University
Aditya Pratap Singh
 
PPTX
Circuits
Hassaan Rahman
 
PPTX
2202NotesSet04v17.pptx NAS NOTES FILTERS
kiran93845
 
PPTX
MathematicalModelling.pptxGFYDTUSRYJETDTUYR
Dhaifallaharef
 
PPTX
Chapter 2 Network analysis and synthesis.pptx
ephremshiferawww
 
PPT
Circuits
SajidKhan933601
 
PPT
Hamid
Rana Hamid
 
PPT
Finite State Machine by M. Arokiasamy
Mark Arokiasamy
 
PDF
1_5_2020_network_initial_conditions_60_days_crash_course_for_iPATE.pdf
sivaenotes
 
PDF
basic-electrical-engineering-all-unit-notes.pdf
LAXMISFXEET036
 
PPTX
Chep 03 Electrical transient
Piyush Tandel
 
PPTX
Network anallysis ppt networks theorems
satyaasai2904
 
PPTX
Network analysis lecture 1.pptx
CHHAYAKHANDELWAL
 
Initial Conditions
Smit Shah
 
Initial Conditions
Soham Gajjar
 
Initial condition
Ravi Patel
 
Lecture slides Ist & 2nd Order Circuits[282].pdf
sami717280
 
Second order circuits linear circuit analysis
ZulqarnainEngineerin
 
RL RC _src - Basic electric theory .pptx
happycocoman
 
Assignmentl3 solutions
Om Prakash Bankolia
 
Step respponse of rlc circuit by Aditya Pratap Singh Delhi University
Aditya Pratap Singh
 
Circuits
Hassaan Rahman
 
2202NotesSet04v17.pptx NAS NOTES FILTERS
kiran93845
 
MathematicalModelling.pptxGFYDTUSRYJETDTUYR
Dhaifallaharef
 
Chapter 2 Network analysis and synthesis.pptx
ephremshiferawww
 
Circuits
SajidKhan933601
 
Hamid
Rana Hamid
 
Finite State Machine by M. Arokiasamy
Mark Arokiasamy
 
1_5_2020_network_initial_conditions_60_days_crash_course_for_iPATE.pdf
sivaenotes
 
basic-electrical-engineering-all-unit-notes.pdf
LAXMISFXEET036
 
Chep 03 Electrical transient
Piyush Tandel
 
Network anallysis ppt networks theorems
satyaasai2904
 
Network analysis lecture 1.pptx
CHHAYAKHANDELWAL
 
Ad

More from Jayanshu Gundaniya (15)

PPTX
Erbium Doped Fiber Amplifier (EDFA)
Jayanshu Gundaniya
 
PPTX
Three Phase to Three phase Cycloconverter
Jayanshu Gundaniya
 
PPTX
Fourier Series for Continuous Time & Discrete Time Signals
Jayanshu Gundaniya
 
PPT
Comparison of A, B & C Power Amplifiers
Jayanshu Gundaniya
 
PPT
Multiplexers & Demultiplexers
Jayanshu Gundaniya
 
PPT
First order non-linear partial differential equation & its applications
Jayanshu Gundaniya
 
PPT
Engineering Mathematics - Total derivatives, chain rule and derivative of imp...
Jayanshu Gundaniya
 
PPT
Engineering Graphics - Projection of points and lines
Jayanshu Gundaniya
 
PPT
Internal expanding shoe brake short presentation
Jayanshu Gundaniya
 
PPT
Hydrological cycle
Jayanshu Gundaniya
 
PPT
Ecology and ecosystem
Jayanshu Gundaniya
 
PPT
Basics of pointer, pointer expressions, pointer to pointer and pointer in fun...
Jayanshu Gundaniya
 
PPT
Architectural acoustics topics and remedies - short presentation
Jayanshu Gundaniya
 
PPT
Superconductors and Superconductivity
Jayanshu Gundaniya
 
PPTX
Superposition theorem
Jayanshu Gundaniya
 
Erbium Doped Fiber Amplifier (EDFA)
Jayanshu Gundaniya
 
Three Phase to Three phase Cycloconverter
Jayanshu Gundaniya
 
Fourier Series for Continuous Time & Discrete Time Signals
Jayanshu Gundaniya
 
Comparison of A, B & C Power Amplifiers
Jayanshu Gundaniya
 
Multiplexers & Demultiplexers
Jayanshu Gundaniya
 
First order non-linear partial differential equation & its applications
Jayanshu Gundaniya
 
Engineering Mathematics - Total derivatives, chain rule and derivative of imp...
Jayanshu Gundaniya
 
Engineering Graphics - Projection of points and lines
Jayanshu Gundaniya
 
Internal expanding shoe brake short presentation
Jayanshu Gundaniya
 
Hydrological cycle
Jayanshu Gundaniya
 
Ecology and ecosystem
Jayanshu Gundaniya
 
Basics of pointer, pointer expressions, pointer to pointer and pointer in fun...
Jayanshu Gundaniya
 
Architectural acoustics topics and remedies - short presentation
Jayanshu Gundaniya
 
Superconductors and Superconductivity
Jayanshu Gundaniya
 
Superposition theorem
Jayanshu Gundaniya
 

Recently uploaded (20)

PDF
Zero Carbon Building Performance standard
BassemOsman1
 
PPTX
Module2 Data Base Design- ER and NF.pptx
gomathisankariv2
 
PDF
Construction of a Thermal Vacuum Chamber for Environment Test of Triple CubeS...
2208441
 
PDF
EVS+PRESENTATIONS EVS+PRESENTATIONS like
saiyedaqib429
 
PPTX
MULTI LEVEL DATA TRACKING USING COOJA.pptx
dollysharma12ab
 
PDF
FLEX-LNG-Company-Presentation-Nov-2017.pdf
jbloggzs
 
PDF
AI-Driven IoT-Enabled UAV Inspection Framework for Predictive Maintenance and...
ijcncjournal019
 
PPTX
IoT_Smart_Agriculture_Presentations.pptx
poojakumari696707
 
PDF
2010_Book_EnvironmentalBioengineering (1).pdf
EmilianoRodriguezTll
 
PDF
Chad Ayach - A Versatile Aerospace Professional
Chad Ayach
 
PPT
Understanding the Key Components and Parts of a Drone System.ppt
Siva Reddy
 
PPTX
Victory Precisions_Supplier Profile.pptx
victoryprecisions199
 
PDF
Machine Learning All topics Covers In This Single Slides
AmritTiwari19
 
PPTX
22PCOAM21 Session 1 Data Management.pptx
Guru Nanak Technical Institutions
 
PDF
Packaging Tips for Stainless Steel Tubes and Pipes
heavymetalsandtubes
 
PPTX
Inventory management chapter in automation and robotics.
atisht0104
 
PDF
All chapters of Strength of materials.ppt
girmabiniyam1234
 
PDF
Biodegradable Plastics: Innovations and Market Potential (www.kiu.ac.ug)
publication11
 
PDF
Introduction to Ship Engine Room Systems.pdf
Mahmoud Moghtaderi
 
PDF
20ME702-Mechatronics-UNIT-1,UNIT-2,UNIT-3,UNIT-4,UNIT-5, 2025-2026
Mohanumar S
 
Zero Carbon Building Performance standard
BassemOsman1
 
Module2 Data Base Design- ER and NF.pptx
gomathisankariv2
 
Construction of a Thermal Vacuum Chamber for Environment Test of Triple CubeS...
2208441
 
EVS+PRESENTATIONS EVS+PRESENTATIONS like
saiyedaqib429
 
MULTI LEVEL DATA TRACKING USING COOJA.pptx
dollysharma12ab
 
FLEX-LNG-Company-Presentation-Nov-2017.pdf
jbloggzs
 
AI-Driven IoT-Enabled UAV Inspection Framework for Predictive Maintenance and...
ijcncjournal019
 
IoT_Smart_Agriculture_Presentations.pptx
poojakumari696707
 
2010_Book_EnvironmentalBioengineering (1).pdf
EmilianoRodriguezTll
 
Chad Ayach - A Versatile Aerospace Professional
Chad Ayach
 
Understanding the Key Components and Parts of a Drone System.ppt
Siva Reddy
 
Victory Precisions_Supplier Profile.pptx
victoryprecisions199
 
Machine Learning All topics Covers In This Single Slides
AmritTiwari19
 
22PCOAM21 Session 1 Data Management.pptx
Guru Nanak Technical Institutions
 
Packaging Tips for Stainless Steel Tubes and Pipes
heavymetalsandtubes
 
Inventory management chapter in automation and robotics.
atisht0104
 
All chapters of Strength of materials.ppt
girmabiniyam1234
 
Biodegradable Plastics: Innovations and Market Potential (www.kiu.ac.ug)
publication11
 
Introduction to Ship Engine Room Systems.pdf
Mahmoud Moghtaderi
 
20ME702-Mechatronics-UNIT-1,UNIT-2,UNIT-3,UNIT-4,UNIT-5, 2025-2026
Mohanumar S
 

Initial Conditions of Resistor, Inductor & Capacitor

  • 1. INITIAL CONDITIONS : WHY TO STUDY • Differential Equations written for a network may contain arbitrary constants equal to the order of the differential equations. • The reason for studying initial conditions is to find the value of arbitrary constants that appear in the general solution of differential equations written for a given network.
  • 2. INITIAL CONDITIONS • In Initial conditions, we find the change in selected variables in a circuit when one or more switches are moved from open to closed positions or vice versa. t=0- indicates the time just before changing the position of the switch t=0 indicates the time when the position of switch is changed t=0+ indicates the time immediately after changing the position of switch
  • 3. INITIAL CONDITIONS • Initial condition focuses solely on the current and voltages of energy storing elements (inductor and capacitor) as they will determine the circuit behavior at t>0. • PAST HISTORY OF THE CIRCUIT WILL SHOW UP AS THE CAPACITOR VOLTAGES AND INDUCTOR CURRENTS
  • 4. INITIAL CONDITIONS 1. RESISTOR  The voltage current relation of an ideal resistance is V=R*I  From this equation it can be concluded that the instantaneous current flowing through the resistor changes if the instantaneous voltage across it changes & vice versa  The past voltage or current values have no effect on the present or future working of the resistor i.e.. It’s resistance remains the same irrespective of the past conditions
  • 5. INITIAL CONDITIONS 2. INDUCTOR  The expression for current through the inductor is given by
  • 6. INITIAL CONDITIONS Hence if i(0- )=0A , then i(0+ )=0A So we can visualize inductor as a open circuit at t=0+
  • 7. INITIAL CONDITIONS • If i(0- )=I0 , then i(0+ )=I0 i.e. the inductor can be thought as a current source of I0 as shown
  • 8. INITIAL CONDITIONS FINAL CONDITIONS :  From the basic relationship V= L*(di/dt) We can state that V=0 in steady state conditions at t= as (di/dt)=0 due to constant current
  • 9. INITIAL CONDITIONS 3. CAPACITOR  The expression for voltage across the capacitor is given by
  • 10. INITIAL CONDITIONS If V(0- )=0V , then V(0+ )=0V indicating the capacitor as a short circuit
  • 11. INITIAL CONDITIONS If V(0- )= V volts, then the capacitor can be visualized as a voltage source of V volts
  • 12. INITIAL CONDITIONS • Final Conditions The current across the capacitor is given by the equation i=C*(dv/dt) which indicates that i=0A in steady state at t= due to capacitor being fully charged.
  • 13. INITIAL CONDITION EXAMPLE-1 : In the network shown in the figure the switch is closed at t=0. Determine i, (di/dt) and (d2 i/dt2 ) at t=0+ . At t=0- , the switch is Closed. Due to which il(0- )=0A Vc(0- )=0V
  • 14. INITIAL CONDITION At t=0+ the circuit is From the circuit il(0+ )=0A Vc(0+ )=0V
  • 15. INITIAL CONDITION • Writing KVL clockwise for the circuit Putting t=0+ in equation (2)
  • 16. INITIAL CONDITION • Differentiating equation (1) with respect to time
  • 17. INITIAL CONDITION  Example 2: The position of switch was changed from 1 to 2 at t=0. Steady State was achieved when the switch was at position 1. Find i, (di/dt) & (d2 i/dt2 ) at t=0+
  • 18. INITIAL CONDITION At t=0- , the circuit is shown in figure The inductor is in steady state so it is assumed to be shorted. So the current through it is il(0- )=20/10=2A Vc(0- )=0V
  • 19. INITIAL CONDITION So at t=0+ , the switch is at position 2 Here the Inductor behaves as a current source of 2A. The circuit is shown below il(0+ )=2A Vc(0+ )=0V