SlideShare a Scribd company logo
Internal Resistance of cell &
   Combinations of Cells
            01.06.09

  By R. S. Saini
                           (M.Sc. Physics, M.Ed.)
Kendriya Vidyalaya, Sector 47, Chandigarh

          9417071540
Sources of emf:

The electro motive force is the maximum potential difference between the
two electrodes of the cell when no current is drawn from the cell.

Comparison of EMF and P.D:
     EMF                                Potential Difference
 1   EMF is the maximum potential       P.D is the difference of potentials
     difference between the two         between any two points in a closed
     electrodes of the cell when no     circuit.
     current is drawn from the cell
     i.e. when the circuit is open.
 2   It is independent of the           It is proportional to the resistance
     resistance of the circuit.         between the given points.

 3   The term ‘emf’ is used only for    It is measured between any two
     the source of emf.                 points of the circuit.

 4   It is greater than the potential   However, p.d. is greater than emf
     difference between any two         when the cell is being charged.
     points in a circuit.
Internal Resistance of a cell:
The opposition offered by the electrolyte of the cell to the flow of electric
current through it is called the internal resistance of the cell.
Factors affecting Internal Resistance of a cell:
i)   Larger the separation between the electrodes of the cell, more the length
     of the electrolyte through which current has to flow and consequently a
     higher value of internal resistance.
ii) Greater the conductivity of the electrolyte, lesser is the internal resistance
    of the cell. i.e. internal resistance depends on the nature of the electrolyte.
iii) The internal resistance of a cell is inversely proportional to the common
     area of the electrodes dipping in the electrolyte.
iv) The internal resistance of a cell depends on the nature of the electrodes.
    E =V+v
       = IR + Ir                                              E r
       = I (R + r)                                               v
                                                     I                      I
     I = E / (R + r)
                                                               R
     This relation is called circuit equation.
                                                                V
Internal Resistance of a cell in terms of E,V and R:

      E =V+v                                                            E r
         = V + Ir
      Ir = E - V                                                         v
                                                              I                  I
      Dividing by IR = V,                                               R

      Ir       E–V                       E                               V
           =                      r =(           - 1) R
      IR           V                     V


Determination of Internal Resistance of a cell by voltmeter method:
                       V                                      V
               +                                          +

                           r                                      r

                                             I                               I
                       R.B (R)                                R.B (R)

           K                                     K
  Open circuit (No current is drawn)     Closed circuit (Current is drawn)
  EMF (E) is measured                    Potential Difference (V) is measured
Cells in Series combination:
Cells are connected in series when they are joined end to end so that the
same quantity of electricity must flow through each cell.
NOTE:
                                                    E r            E r           E r
1. The emf of the battery is the
   sum of the individual emfs
                                      I                                                          I
2. The current in each cell is the
   same and is identical with the                                   R
   current in the entire
   arrangement.                                                     V
3. The total internal resistance of
   the battery is the sum of the
   individual internal resistances.

  Total emf of the battery                       = nE       (for n no. of identical cells)
  Total Internal resistance of the battery = nr
  Total resistance of the circuit                = nr + R

                            (i) If R << nr, then I = E / r (ii) If nr << R, then I = n (E / R)
                   nE
   Current I =               Conclusion: When internal resistance is negligible in
                 nr + R      comparison to the external resistance, then the cells are
                             connected in series to get maximum current.
Cells in Parallel combination:
Cells are said to be connected in parallel when they are joined positive to
positive and negative to negative such that current is divided between the cells.
                                                                              E r
NOTE:
1. The emf of the battery is the same as that of a
   single cell.
                                                                              E r
2. The current in the external circuit is divided equally
   among the cells.
3. The reciprocal of the total internal resistance is the                     E r
   sum of the reciprocals of the individual internal            I                                 I
   resistances.

Total emf of the battery                        = E                             R

Total Internal resistance of the battery = r / n                                V
Total resistance of the circuit                = (r / n) + R


                            (i) If R << r/n, then I = n(E / r) (ii) If r/n << R, then I = E / R
                   nE
   Current I =               Conclusion: When external resistance is negligible in
                  nR + r     comparison to the internal resistance, then the cells are
                             connected in parallel to get maximum current.
Mixed Grouping
Cells are said to be in mixed grouping if are
connected in the manner as shown.
Mixed Grouping




Let n be the no. of cells in series in each row and m be
the no. of such rows. Let E be the e.m.f. of each cell
and ‘r’ be the internal resistance of each cell.
In each row, there are n cells in series, therefore their
total resistance is ‘nr’ and total e.m.f. in nE.
Thus are ‘m’ rows of cells in parallel, therefore total
internal resistance of all the cells is given by
            1 1 1         1                       m
              = + +−−−−−−         ( m terms ) =
            rp nr nr      nr                      nr
Mixed Grouping
                                           nr
Hence total resistance in the circuit is =
                                           m
and effective e.m.f. is = nE
                           nE    mnE
Hence total current    I=      =        − − − − − (1)
                             nr mR + nr
                          R+
                             m
For current I to be maximum mR + nr should be
minimum which can be proved to be minimum when
mR = nr as follows
Mixed Grouping
                         2        2
mR + nr =   (  ) + ( nr )
                mR
        2                2
= ( mR ) + ( nr ) − 2 ml nr + 2       ml nr
                    2
= ( mR − nr ) + 2 mR nr

Which is minimum when
   mR − nr = 0 or mR = nr
And maximum current is given by
                          mE nE
                I max   =   =
                          2r 2R

More Related Content

What's hot

ELECTRIC POTENTIAL
ELECTRIC POTENTIALELECTRIC POTENTIAL
ELECTRIC POTENTIAL
Sheeba vinilan
 
Alternating Current
Alternating CurrentAlternating Current
Alternating Current
Priyanka Jakhar
 
Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2
Self-employed
 
Magnetic Effects Of Current Class 12 Part-3
Magnetic Effects Of Current Class 12 Part-3Magnetic Effects Of Current Class 12 Part-3
Magnetic Effects Of Current Class 12 Part-3
Self-employed
 
Semiconductor Devices Class 12 Part-2
Semiconductor Devices Class 12 Part-2Semiconductor Devices Class 12 Part-2
Semiconductor Devices Class 12 Part-2
Self-employed
 
Lecture-20.ppt
Lecture-20.pptLecture-20.ppt
Lecture-20.ppt
MAXWELLShorts
 
Current Electricity Class 12 Part-1
Current Electricity Class 12 Part-1Current Electricity Class 12 Part-1
Current Electricity Class 12 Part-1
Self-employed
 
Electric Field
Electric FieldElectric Field
Electric Field
umarjamil10000
 
Current electricity
Current electricityCurrent electricity
Current electricity
Natasia Gouws
 
Electromagnetic Induction Class 12
Electromagnetic Induction Class 12 Electromagnetic Induction Class 12
Electromagnetic Induction Class 12
Self-employed
 
Electrostatics Class 12- Part 3
Electrostatics Class 12- Part 3Electrostatics Class 12- Part 3
Electrostatics Class 12- Part 3
Self-employed
 
Lorentz Force Magnetic Force on a moving charge in uniform Electric and Mag...
Lorentz Force  Magnetic Force on a moving charge in uniform  Electric and Mag...Lorentz Force  Magnetic Force on a moving charge in uniform  Electric and Mag...
Lorentz Force Magnetic Force on a moving charge in uniform Electric and Mag...
Priyanka Jakhar
 
Internal resistance
Internal resistanceInternal resistance
Internal resistance
amckaytghs
 
self inductance , mutual inductance and coeffecient of coupling
self inductance , mutual inductance and coeffecient of couplingself inductance , mutual inductance and coeffecient of coupling
self inductance , mutual inductance and coeffecient of coupling
saahil kshatriya
 
AP Physics - Chapter 18 Powerpoint
AP Physics - Chapter 18 PowerpointAP Physics - Chapter 18 Powerpoint
AP Physics - Chapter 18 Powerpoint
Mrreynon
 
Capacitance
CapacitanceCapacitance
Capacitance
stooty s
 
Ch 12 (atoms)
Ch 12 (atoms)Ch 12 (atoms)
Ch 12 (atoms)
Abhijeet Kumar
 
Semiconductor Devices Class 12 Part-4
Semiconductor Devices Class 12 Part-4Semiconductor Devices Class 12 Part-4
Semiconductor Devices Class 12 Part-4
Self-employed
 
Physics investigatory project
Physics investigatory projectPhysics investigatory project
Physics investigatory project
Shivalik school
 
cell.ppt
cell.pptcell.ppt
cell.ppt
Priyanka Jakhar
 

What's hot (20)

ELECTRIC POTENTIAL
ELECTRIC POTENTIALELECTRIC POTENTIAL
ELECTRIC POTENTIAL
 
Alternating Current
Alternating CurrentAlternating Current
Alternating Current
 
Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2Electrostatics Class 12- Part 2
Electrostatics Class 12- Part 2
 
Magnetic Effects Of Current Class 12 Part-3
Magnetic Effects Of Current Class 12 Part-3Magnetic Effects Of Current Class 12 Part-3
Magnetic Effects Of Current Class 12 Part-3
 
Semiconductor Devices Class 12 Part-2
Semiconductor Devices Class 12 Part-2Semiconductor Devices Class 12 Part-2
Semiconductor Devices Class 12 Part-2
 
Lecture-20.ppt
Lecture-20.pptLecture-20.ppt
Lecture-20.ppt
 
Current Electricity Class 12 Part-1
Current Electricity Class 12 Part-1Current Electricity Class 12 Part-1
Current Electricity Class 12 Part-1
 
Electric Field
Electric FieldElectric Field
Electric Field
 
Current electricity
Current electricityCurrent electricity
Current electricity
 
Electromagnetic Induction Class 12
Electromagnetic Induction Class 12 Electromagnetic Induction Class 12
Electromagnetic Induction Class 12
 
Electrostatics Class 12- Part 3
Electrostatics Class 12- Part 3Electrostatics Class 12- Part 3
Electrostatics Class 12- Part 3
 
Lorentz Force Magnetic Force on a moving charge in uniform Electric and Mag...
Lorentz Force  Magnetic Force on a moving charge in uniform  Electric and Mag...Lorentz Force  Magnetic Force on a moving charge in uniform  Electric and Mag...
Lorentz Force Magnetic Force on a moving charge in uniform Electric and Mag...
 
Internal resistance
Internal resistanceInternal resistance
Internal resistance
 
self inductance , mutual inductance and coeffecient of coupling
self inductance , mutual inductance and coeffecient of couplingself inductance , mutual inductance and coeffecient of coupling
self inductance , mutual inductance and coeffecient of coupling
 
AP Physics - Chapter 18 Powerpoint
AP Physics - Chapter 18 PowerpointAP Physics - Chapter 18 Powerpoint
AP Physics - Chapter 18 Powerpoint
 
Capacitance
CapacitanceCapacitance
Capacitance
 
Ch 12 (atoms)
Ch 12 (atoms)Ch 12 (atoms)
Ch 12 (atoms)
 
Semiconductor Devices Class 12 Part-4
Semiconductor Devices Class 12 Part-4Semiconductor Devices Class 12 Part-4
Semiconductor Devices Class 12 Part-4
 
Physics investigatory project
Physics investigatory projectPhysics investigatory project
Physics investigatory project
 
cell.ppt
cell.pptcell.ppt
cell.ppt
 

Similar to Phy1

2currentelectricity1-140315124205-phpapp01
2currentelectricity1-140315124205-phpapp012currentelectricity1-140315124205-phpapp01
2currentelectricity1-140315124205-phpapp01
Aman Meena
 
2currentelectricity1-140315124205-phpapp01 (1).pdf
2currentelectricity1-140315124205-phpapp01 (1).pdf2currentelectricity1-140315124205-phpapp01 (1).pdf
2currentelectricity1-140315124205-phpapp01 (1).pdf
2kGamer3
 
Class 12th physics current electricity ppt
Class 12th physics current electricity ppt Class 12th physics current electricity ppt
Class 12th physics current electricity ppt
Arpit Meena
 
2_current_electricity_1.pptnefipnipdannaffkn
2_current_electricity_1.pptnefipnipdannaffkn2_current_electricity_1.pptnefipnipdannaffkn
2_current_electricity_1.pptnefipnipdannaffkn
Karthik537368
 
2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD
Karthik537368
 
2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD
Karthik537368
 
2_current_electricity_1.ppt
2_current_electricity_1.ppt2_current_electricity_1.ppt
2_current_electricity_1.ppt
TayyabShabir
 
2_current_electricity_1.ppt
2_current_electricity_1.ppt2_current_electricity_1.ppt
2_current_electricity_1.ppt
TSANROSEBASTIN
 
current electricity PHYSICS CHAPTER 2.ppt
current electricity     PHYSICS CHAPTER 2.pptcurrent electricity     PHYSICS CHAPTER 2.ppt
current electricity PHYSICS CHAPTER 2.ppt
HarshPawar30
 
currentelectricity.pptx
currentelectricity.pptxcurrentelectricity.pptx
currentelectricity.pptx
RemyaRajesh10
 
project EMF AND BATTERY.pdf CLAS 12TH TOPIC
project EMF AND BATTERY.pdf CLAS 12TH TOPICproject EMF AND BATTERY.pdf CLAS 12TH TOPIC
project EMF AND BATTERY.pdf CLAS 12TH TOPIC
AditiGupta109884
 
Electric circuits grade 10
Electric circuits grade 10Electric circuits grade 10
Electric circuits grade 10
Siyavula
 
Direct Current QA 9
Direct Current QA 9Direct Current QA 9
Direct Current QA 9
Lakshmikanta Satapathy
 
factors affecting internal resistance/emf of the cell
factors affecting internal resistance/emf of the cellfactors affecting internal resistance/emf of the cell
factors affecting internal resistance/emf of the cell
Yogesh Baghel
 
Ee study notes
Ee study notesEe study notes
Ee study notes
CK Yang
 
C.12 PHYSICS CURRENT ELECTRICITY notes.pdf
C.12 PHYSICS CURRENT ELECTRICITY notes.pdfC.12 PHYSICS CURRENT ELECTRICITY notes.pdf
C.12 PHYSICS CURRENT ELECTRICITY notes.pdf
ZiauddinKhan34
 
Direct Current Theory 4
Direct Current Theory 4Direct Current Theory 4
Direct Current Theory 4
Lakshmikanta Satapathy
 
Chapter1: Electricity
Chapter1: ElectricityChapter1: Electricity
Chapter1: Electricity
marjerin
 
Cells in Series and in Parallel | Physics
Cells in Series and in Parallel | PhysicsCells in Series and in Parallel | Physics
Cells in Series and in Parallel | Physics
askIITians - Creating Engineers & Doctors
 
Find_out_the_effective_resistance.pptx
Find_out_the_effective_resistance.pptxFind_out_the_effective_resistance.pptx
Find_out_the_effective_resistance.pptx
gracelmj
 

Similar to Phy1 (20)

2currentelectricity1-140315124205-phpapp01
2currentelectricity1-140315124205-phpapp012currentelectricity1-140315124205-phpapp01
2currentelectricity1-140315124205-phpapp01
 
2currentelectricity1-140315124205-phpapp01 (1).pdf
2currentelectricity1-140315124205-phpapp01 (1).pdf2currentelectricity1-140315124205-phpapp01 (1).pdf
2currentelectricity1-140315124205-phpapp01 (1).pdf
 
Class 12th physics current electricity ppt
Class 12th physics current electricity ppt Class 12th physics current electricity ppt
Class 12th physics current electricity ppt
 
2_current_electricity_1.pptnefipnipdannaffkn
2_current_electricity_1.pptnefipnipdannaffkn2_current_electricity_1.pptnefipnipdannaffkn
2_current_electricity_1.pptnefipnipdannaffkn
 
2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD
 
2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD2_current_electricity_1.pptcdasdDdDddddddD
2_current_electricity_1.pptcdasdDdDddddddD
 
2_current_electricity_1.ppt
2_current_electricity_1.ppt2_current_electricity_1.ppt
2_current_electricity_1.ppt
 
2_current_electricity_1.ppt
2_current_electricity_1.ppt2_current_electricity_1.ppt
2_current_electricity_1.ppt
 
current electricity PHYSICS CHAPTER 2.ppt
current electricity     PHYSICS CHAPTER 2.pptcurrent electricity     PHYSICS CHAPTER 2.ppt
current electricity PHYSICS CHAPTER 2.ppt
 
currentelectricity.pptx
currentelectricity.pptxcurrentelectricity.pptx
currentelectricity.pptx
 
project EMF AND BATTERY.pdf CLAS 12TH TOPIC
project EMF AND BATTERY.pdf CLAS 12TH TOPICproject EMF AND BATTERY.pdf CLAS 12TH TOPIC
project EMF AND BATTERY.pdf CLAS 12TH TOPIC
 
Electric circuits grade 10
Electric circuits grade 10Electric circuits grade 10
Electric circuits grade 10
 
Direct Current QA 9
Direct Current QA 9Direct Current QA 9
Direct Current QA 9
 
factors affecting internal resistance/emf of the cell
factors affecting internal resistance/emf of the cellfactors affecting internal resistance/emf of the cell
factors affecting internal resistance/emf of the cell
 
Ee study notes
Ee study notesEe study notes
Ee study notes
 
C.12 PHYSICS CURRENT ELECTRICITY notes.pdf
C.12 PHYSICS CURRENT ELECTRICITY notes.pdfC.12 PHYSICS CURRENT ELECTRICITY notes.pdf
C.12 PHYSICS CURRENT ELECTRICITY notes.pdf
 
Direct Current Theory 4
Direct Current Theory 4Direct Current Theory 4
Direct Current Theory 4
 
Chapter1: Electricity
Chapter1: ElectricityChapter1: Electricity
Chapter1: Electricity
 
Cells in Series and in Parallel | Physics
Cells in Series and in Parallel | PhysicsCells in Series and in Parallel | Physics
Cells in Series and in Parallel | Physics
 
Find_out_the_effective_resistance.pptx
Find_out_the_effective_resistance.pptxFind_out_the_effective_resistance.pptx
Find_out_the_effective_resistance.pptx
 

Recently uploaded

Snoopy boards the big bow wow musical __
Snoopy boards the big bow wow musical __Snoopy boards the big bow wow musical __
Snoopy boards the big bow wow musical __
catcabrera
 
Modern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
Modern Radio Frequency Access Control Systems: The Key to Efficiency and SafetyModern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
Modern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
AITIX LLC
 
Everything You Need to Know About IPTV Ireland.pdf
Everything You Need to Know About IPTV Ireland.pdfEverything You Need to Know About IPTV Ireland.pdf
Everything You Need to Know About IPTV Ireland.pdf
Xtreame HDTV
 
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
greendigital
 
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
0md20cgg
 
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
mul1kv5w
 
Divertidamente SLIDE muito lindo e criativo, pptx
Divertidamente SLIDE muito lindo e criativo, pptxDivertidamente SLIDE muito lindo e criativo, pptx
Divertidamente SLIDE muito lindo e criativo, pptx
lunaemel03
 
Christian Louboutin: Innovating with Red Soles
Christian Louboutin: Innovating with Red SolesChristian Louboutin: Innovating with Red Soles
Christian Louboutin: Innovating with Red Soles
get joys
 
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
9u08k0x
 
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdfMatt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
Azura Everhart
 
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptxFrom Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
Swing Street Radio
 
I Know Dino Trivia: Part 3. Test your dino knowledge
I Know Dino Trivia: Part 3. Test your dino knowledgeI Know Dino Trivia: Part 3. Test your dino knowledge
I Know Dino Trivia: Part 3. Test your dino knowledge
Sabrina Ricci
 
Barbie Movie Review - The Astras.pdfffff
Barbie Movie Review - The Astras.pdfffffBarbie Movie Review - The Astras.pdfffff
Barbie Movie Review - The Astras.pdfffff
theastras43
 
DIGIDEVTV A New area of OTT Distribution
DIGIDEVTV  A New area of OTT DistributionDIGIDEVTV  A New area of OTT Distribution
DIGIDEVTV A New area of OTT Distribution
joeqsm
 
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdfUnveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
kenid14983
 
Meet Dinah Mattingly – Larry Bird’s Partner in Life and Love
Meet Dinah Mattingly – Larry Bird’s Partner in Life and LoveMeet Dinah Mattingly – Larry Bird’s Partner in Life and Love
Meet Dinah Mattingly – Larry Bird’s Partner in Life and Love
get joys
 
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
Mega P
 
Orpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
Orpah Winfrey Dwayne Johnson: Titans of Influence and InspirationOrpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
Orpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
greendigital
 
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting SagaThe Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
greendigital
 
Top IPTV UK Providers of A Comprehensive Review.pdf
Top IPTV UK Providers of A Comprehensive Review.pdfTop IPTV UK Providers of A Comprehensive Review.pdf
Top IPTV UK Providers of A Comprehensive Review.pdf
Xtreame HDTV
 

Recently uploaded (20)

Snoopy boards the big bow wow musical __
Snoopy boards the big bow wow musical __Snoopy boards the big bow wow musical __
Snoopy boards the big bow wow musical __
 
Modern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
Modern Radio Frequency Access Control Systems: The Key to Efficiency and SafetyModern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
Modern Radio Frequency Access Control Systems: The Key to Efficiency and Safety
 
Everything You Need to Know About IPTV Ireland.pdf
Everything You Need to Know About IPTV Ireland.pdfEverything You Need to Know About IPTV Ireland.pdf
Everything You Need to Know About IPTV Ireland.pdf
 
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
The Evolution of the Leonardo DiCaprio Haircut: A Journey Through Style and C...
 
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
定制(uow毕业证书)卧龙岗大学毕业证文凭学位证书原版一模一样
 
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
原版制作(Mercer毕业证书)摩斯大学毕业证在读证明一模一样
 
Divertidamente SLIDE muito lindo e criativo, pptx
Divertidamente SLIDE muito lindo e criativo, pptxDivertidamente SLIDE muito lindo e criativo, pptx
Divertidamente SLIDE muito lindo e criativo, pptx
 
Christian Louboutin: Innovating with Red Soles
Christian Louboutin: Innovating with Red SolesChristian Louboutin: Innovating with Red Soles
Christian Louboutin: Innovating with Red Soles
 
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
哪里买(osu毕业证书)美国俄勒冈州立大学毕业证双学位证书原版一模一样
 
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdfMatt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
Matt Rife Cancels Shows Due to Health Concerns, Reschedules Tour Dates.pdf
 
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptxFrom Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
From Swing Music to Big Band Fame_ 5 Iconic Artists.pptx
 
I Know Dino Trivia: Part 3. Test your dino knowledge
I Know Dino Trivia: Part 3. Test your dino knowledgeI Know Dino Trivia: Part 3. Test your dino knowledge
I Know Dino Trivia: Part 3. Test your dino knowledge
 
Barbie Movie Review - The Astras.pdfffff
Barbie Movie Review - The Astras.pdfffffBarbie Movie Review - The Astras.pdfffff
Barbie Movie Review - The Astras.pdfffff
 
DIGIDEVTV A New area of OTT Distribution
DIGIDEVTV  A New area of OTT DistributionDIGIDEVTV  A New area of OTT Distribution
DIGIDEVTV A New area of OTT Distribution
 
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdfUnveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
Unveiling Paul Haggis Shaping Cinema Through Diversity. .pdf
 
Meet Dinah Mattingly – Larry Bird’s Partner in Life and Love
Meet Dinah Mattingly – Larry Bird’s Partner in Life and LoveMeet Dinah Mattingly – Larry Bird’s Partner in Life and Love
Meet Dinah Mattingly – Larry Bird’s Partner in Life and Love
 
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
_7 OTT App Builders to Support the Development of Your Video Applications_.pdf
 
Orpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
Orpah Winfrey Dwayne Johnson: Titans of Influence and InspirationOrpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
Orpah Winfrey Dwayne Johnson: Titans of Influence and Inspiration
 
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting SagaThe Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
The Unbelievable Tale of Dwayne Johnson Kidnapping: A Riveting Saga
 
Top IPTV UK Providers of A Comprehensive Review.pdf
Top IPTV UK Providers of A Comprehensive Review.pdfTop IPTV UK Providers of A Comprehensive Review.pdf
Top IPTV UK Providers of A Comprehensive Review.pdf
 

Phy1

  • 1. Internal Resistance of cell & Combinations of Cells 01.06.09 By R. S. Saini (M.Sc. Physics, M.Ed.) Kendriya Vidyalaya, Sector 47, Chandigarh 9417071540
  • 2. Sources of emf: The electro motive force is the maximum potential difference between the two electrodes of the cell when no current is drawn from the cell. Comparison of EMF and P.D: EMF Potential Difference 1 EMF is the maximum potential P.D is the difference of potentials difference between the two between any two points in a closed electrodes of the cell when no circuit. current is drawn from the cell i.e. when the circuit is open. 2 It is independent of the It is proportional to the resistance resistance of the circuit. between the given points. 3 The term ‘emf’ is used only for It is measured between any two the source of emf. points of the circuit. 4 It is greater than the potential However, p.d. is greater than emf difference between any two when the cell is being charged. points in a circuit.
  • 3. Internal Resistance of a cell: The opposition offered by the electrolyte of the cell to the flow of electric current through it is called the internal resistance of the cell. Factors affecting Internal Resistance of a cell: i) Larger the separation between the electrodes of the cell, more the length of the electrolyte through which current has to flow and consequently a higher value of internal resistance. ii) Greater the conductivity of the electrolyte, lesser is the internal resistance of the cell. i.e. internal resistance depends on the nature of the electrolyte. iii) The internal resistance of a cell is inversely proportional to the common area of the electrodes dipping in the electrolyte. iv) The internal resistance of a cell depends on the nature of the electrodes. E =V+v = IR + Ir E r = I (R + r) v I I I = E / (R + r) R This relation is called circuit equation. V
  • 4. Internal Resistance of a cell in terms of E,V and R: E =V+v E r = V + Ir Ir = E - V v I I Dividing by IR = V, R Ir E–V E V = r =( - 1) R IR V V Determination of Internal Resistance of a cell by voltmeter method: V V + + r r I I R.B (R) R.B (R) K K Open circuit (No current is drawn) Closed circuit (Current is drawn) EMF (E) is measured Potential Difference (V) is measured
  • 5. Cells in Series combination: Cells are connected in series when they are joined end to end so that the same quantity of electricity must flow through each cell. NOTE: E r E r E r 1. The emf of the battery is the sum of the individual emfs I I 2. The current in each cell is the same and is identical with the R current in the entire arrangement. V 3. The total internal resistance of the battery is the sum of the individual internal resistances. Total emf of the battery = nE (for n no. of identical cells) Total Internal resistance of the battery = nr Total resistance of the circuit = nr + R (i) If R << nr, then I = E / r (ii) If nr << R, then I = n (E / R) nE Current I = Conclusion: When internal resistance is negligible in nr + R comparison to the external resistance, then the cells are connected in series to get maximum current.
  • 6. Cells in Parallel combination: Cells are said to be connected in parallel when they are joined positive to positive and negative to negative such that current is divided between the cells. E r NOTE: 1. The emf of the battery is the same as that of a single cell. E r 2. The current in the external circuit is divided equally among the cells. 3. The reciprocal of the total internal resistance is the E r sum of the reciprocals of the individual internal I I resistances. Total emf of the battery = E R Total Internal resistance of the battery = r / n V Total resistance of the circuit = (r / n) + R (i) If R << r/n, then I = n(E / r) (ii) If r/n << R, then I = E / R nE Current I = Conclusion: When external resistance is negligible in nR + r comparison to the internal resistance, then the cells are connected in parallel to get maximum current.
  • 7. Mixed Grouping Cells are said to be in mixed grouping if are connected in the manner as shown.
  • 8. Mixed Grouping Let n be the no. of cells in series in each row and m be the no. of such rows. Let E be the e.m.f. of each cell and ‘r’ be the internal resistance of each cell. In each row, there are n cells in series, therefore their total resistance is ‘nr’ and total e.m.f. in nE. Thus are ‘m’ rows of cells in parallel, therefore total internal resistance of all the cells is given by 1 1 1 1 m = + +−−−−−− ( m terms ) = rp nr nr nr nr
  • 9. Mixed Grouping nr Hence total resistance in the circuit is = m and effective e.m.f. is = nE nE mnE Hence total current I= = − − − − − (1) nr mR + nr R+ m For current I to be maximum mR + nr should be minimum which can be proved to be minimum when mR = nr as follows
  • 10. Mixed Grouping 2 2 mR + nr = ( ) + ( nr ) mR 2 2 = ( mR ) + ( nr ) − 2 ml nr + 2 ml nr 2 = ( mR − nr ) + 2 mR nr Which is minimum when mR − nr = 0 or mR = nr And maximum current is given by mE nE I max = = 2r 2R