Electrostatic Formula. Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = -------1------------ C 2 4  e o 4  8.85x10.

Slides:



Advertisements
Similar presentations
APPLIED PHYSICS AND CHEMISTRY ELECTRICITY LECTURE 4 Work and Electric Potential.
Advertisements

Ch. 20 Electric Potential and Electric Potential Energy
Ch 29 : Electric Potential and Electric Potential Energy
LECTURE 11 Pick up reading quiz #2 lecture notes for Lecture 11 Course questionnaire Pick up reading quiz #2 lecture notes for Lecture 11 Course questionnaire.
Reading Quiz The voltage (or electric potential) of a battery determines how much work the battery can do on an electric charge. how much net electric.
Unit 2 Day 3: Electric Energy Storage Electric potential energy stored between capacitor plates Work done to add charge to the capacitor plates Energy.
Capacitors Capacitance is the ability of a component to store energy in the form of an electrostatic charge. A Capacitor is a component designed to provide.
Chapter 17 Capacitance and Capacitors! C = q / V V= voltage q = charge
Capacitance and Dielectrics
Capacitors A device storing electrical energy. Capacitor A potential across connected plates causes charge migration until equilibrium VV – + –q+q Charge.
Electric Energy and Current Chapter 18 Electrical Potential Energy- the potential energy between charges at a distance, or between a charge and an electric.
Chapter 26:Capacitance and Dielectrics. Capacitors A capacitor is made up of 2 conductors carrying charges of equal magnitude and opposite sign. The Capacitance.
Objectives: 1. Define and calculate the capacitance of a capacitor. 2. Describe the factors affecting the capacitance of the capacitor. 3. Calculate the.
1 Capacitance and Dielectrics Chapter 27 Physics chapter 27.
Capacitance Definition Parallel Plate Capacitors Cylindrical Capacitor
23. Electrostatic Energy and Capacitors. 2 Topics Capacitors Electrostatic Energy Using Capacitors.
Lecture 8 Friday January 30 Capacitors and Review.
Capacitance Physics Department, New York City College of Technology.
Chapter 18 Electric Energy and Capacitance demonstrations.
Chapter 26 Capacitance and Dielectrics. Concept Question 1.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 13.1 Capacitance and Electric Fields  Introduction  Capacitors and Capacitance.
Chapter 24 Capacitance, Dielectrics, Electric Energy Storage
W. Sautter Electrostatics is the study of the effects of stationary charges on each other in their surroundings. Charges are created by the transfer.
Capacitors A device storing electrical energy. Capacitor A potential across connected plates causes charge migration until equilibrium VV – + –q+q Charge.
Charge Comes in + and – Is quantized elementary charge, e, is charge on 1 electron or 1 proton e =  Coulombs Is conserved total charge remains.
Electric Potential AP Physics Chapter 17. Electric Charge and Electric Field 17.1 Electric Potential Energy and Potential Difference.
1 16 Overview work, energy, voltage relation between field and voltage capacitance homework: 4, 8, 9, 13, 19, 40, 41, 55, 69, 82, 95, 97.
Electric Potential and Electric Energy; Capacitance Adapted from Giancoli Physics.
ELECTRIC POTENTIAL ENERGY AND ELECTRIC POTENTIAL POTENTIAL ENERGY ELECTRIC POTENTIAL WORK-ENERGY THEOREM CAPACITANCE COMBINATIONS OF CAPACITORS STORED.
How many different ways can a test charge be forced to the right in the diagram? Welcome to a Great Physics Day!
Chapter 18.2 Review Capacitance and Potential. 1. A 5 μF capacitor is connected to a 12 volt battery. What is the potential difference across the plates.
A uniform electric field is an electric field in which the field strength does not vary. This gives constant force a constant force on any charge that.
Chapter 18 Pretest Capacitance and Potential. 1. The amount of charge that can be placed on a capacitor does not depend on: A) the area of the plates,
1/25/2008 J.Velkovska 1 PHYS117B: Lecture 8 More about electric potential  Equipotential lines  Relation between E and V Capacitance.
Lecture 06 - Inductors and Capacitors
Capacitance. Characteristics of a Capacitor No Dielectric Uniform Electric Field d Area Note: Net charge of the system.
Electric Potential and Energy. Objectives Define work and relate it to energy Define electric potential difference, and relate it to the work done on.
1 Capacitance and Capacitors Capacitance:  Any volume (material) that has net charge in it produces electric potential around it (Gauss’ Law).  The ratio.
Fields in Parallel Plates- Capacitors Physics Mrs. Coyle.
Physics 2102 Jonathan Dowling Physics 2102 Lecture 8 Capacitors II.
Today5/2  Questions?  E-Fields and Potential Difference (review)
Electrostatic Energy and Capacitance. Chapter Overview: b Electrostatic Potential Energy: 25-1 b Defining Capacitance: 25-2 b Electrostatic Energy and.
Ch 17: Electric Potential Ch 17 introduces the idea of electric potential (also called Voltage)
Capacitors Physics 1161: Lecture 05 Textbook Sections 20-5 – 20-6.
An electric force of 4.5 x N is measured between two particles. One particle has a charge of 2.0 x C & the other has a charge of 3.0 x
What charge exists on a 30 μF capacitor (fully charged) with a 120 V potential difference between its plates and what is the energy stored? Ans: 3.6.
Objectives: 1. Define and calculate the capacitance of a capacitor. 2. Describe the factors affecting the capacitance of the capacitor. 3. Calculate the.
Objectives: 1. Define and calculate the capacitance of a capacitor. 2. Describe the factors affecting the capacitance of the capacitor. 3. Calculate the.
Capacitors A capacitor is a device that has the ability “capacity” to store electric charge and energy.
Physics 102: Lecture 4, Slide 1 Capacitors! Physics 102: Lecture 04 Today’s lecture will cover Textbook Sections , , 6.
ELECTRIC POTENTIAL ENERGY and the ELECTRIC POTENTIAL.
Chapter 25 Capacitance In this chapter we will cover the following topics: -Capacitance C of a system of two isolated conductors.
Chapter 25 Capacitance In this chapter we will cover the following topics: -Capacitance C of a system of two isolated conductors.
Plan for Today (AP Physics I)
Chapter 11 Capacitance.
Chapter 18.2 Capacitance and Potential
ENERGY STORED BY A CAPACITOR
Electrostatics Forces and Fields
Applications of Coulomb’s Law
Electric Potential AP Physics Chapter 17.
Key Points from Chapter 30
Chapter 18 Pretest Capacitance and Potential
Lecture 09 - Inductors and Capacitors
Introduction to Capacitance
Charge Comes in + and – Is quantized Is conserved
Capacitors.
What charge exists on a 30 μF capacitor (fully charged) with a 120 V potential difference between its plates and what is the energy stored? Ans: 3.6.
Electrical Energy & Capacitance Pgs
Physics 1161: Lecture 06 Capacitors Textbook Sections 20-5 – 20-6.
Starter (5 mins): An object with 25 x 10-6 C of charge is placed in an electric field (electric field strength = 3000 NC-1). Define ‘electric field’
Presentation transcript:

Electrostatic Formula

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Force F = 1 q 1 q 2 = k q 1 q 2 4  e o r 2 r 2 k = 9.0x10 9 N m 2 = 1 = C 2 4  e o 4  8.85x C 2 N m 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field associated with point charges E = F q F = kqq therefore E = Kqq therefore E =kq r 2 r 2 q r 2 Vector sum – x components, y components, sum of x components, sum of y components, pythagorean theorem, and inv tan of (sum of y )/(sum of x )

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E q d

Electric Field Associated with Parallel Plates The electric field is uniform between plates Work is required to move +q from the – to + W=Fd W=qEd W=qKqd W=Kqq W = Kq W =V=Joules= Electric Potential d 2 d q d q Coulomb W=qEd W = Ed V = Ed V = E = Volts q d meter

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance C = Q V C = KA  o d K= dielectric constant A = area in m 2    x C 2 N m 2 d = distance between plates in m

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance W = QV = U ( Potential energy stored ) For a capacitor U = ½ QV since it is easier to add charge at first and progressively gets more difficult C = Q CV = Q therefore U =1/2 QV= ½ CV 2 V C = Q V = Q therefore U = ½ QV = ½ Q 2 V C C

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance C parallel = C 1 +C 2 +C 3 2F4F6F2F4F6F 12  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 12x10 -6 F (3V) = 36x10 -6 C or 3.6x10 -5 Q What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 12x10 -6 F(3V) 2 = U=1.08x10 -4 J What is the charged stored on each of the capacitors? CV=Q= 2x10 -6 F (3V) = 6x10 -6 C CV=Q= 4x10 -6 F (3V) = 12x10 -6 C or 1.2x10 -5 Q CV=Q= 2x10 -6 F (3V) = 18x10 -6 C or 1.8x10 -5 Q

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11=1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11=1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11=1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11=1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J

Capacitance 1 = C series C 1 C 2 C 3 2  F 4  F 6  F 1/C = 1/2  F 1/4  F + 1/6  F 1/C = 11/12  F = 12  F/11= 1.09  F 3 V What is the total charge stored in the system? C = Q V CV = Q = 1.09x10 -6 F (3V) = 3.27x10 -6 C What is the energy stored in the system? U=1/2 QV U = ½ CV 2 U= ½ 3.27x10 -6 F(3V) 2 = U=1.47x10 -5 J