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PHYS.1440 Lecture 11 A.Danylov Department of Physics and Applied Physics Lecture 11 Chapter 26 Capacitors in Series and Parallel Physics II Is there life before coffee? Hmm! 8am Physics class triggers philosophical questions Course website: https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

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  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Lecture 11

    Chapter 26

    Capacitorsin Series and Parallel

    Physics II

    Is there life before coffee?Hmm! 8am Physics class triggers

    philosophical questions

    Course website:https://sites.uml.edu/andriy-danylov/teaching/physics-ii/

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Today we are going to discuss:

    Chapter 26:

    Section 26.5

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Parallel-plate capacitor

    In its simplest form, a capacitor consists of a pair of parallel metal plates separated by air/insulating material.

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Parallel-plate capacitor

    Let’s find capacitance of a parallel-plate capacitor

    Capacitance is a purely geometric property of two electrodes because it depends only on their surface area and spacing.

    π‘ͺ β‰π‘ΈπœŸπ‘½π‘ͺ

    π‘ͺπœΊπŸŽπ‘¨π’…

    E

    d

    Aarea

    +Q–Q

    The electric field between the plates is Ξ· - surface charge density

    𝑄 πœ€ 𝐴𝐸

    πΈπœ‚πœ€

    π›₯𝑉 𝐸𝑑 (Eq.25.26)The potential difference between plates:

    We need to find Q and Ξ”V:

    𝐢 ≝𝑄π›₯𝑉 =

    This gives the capacitance:

    πœ‚π‘„π΄

    π‘„πœ€ 𝐴

  • Sincethebatterystaysconnected,thepotentialdifference

    mustremainconstant! (A, B and E are out)+Q –Q

    A parallel-plate capacitor initially has avoltage of 400 V and stays connected to thebattery. If the plate spacing is nowdoubled, what happens?

    A) the voltage decreases

    B) the voltage increases

    C) the charge decreases

    D) the charge increases

    E) both voltage and charge change

    ConcepTest Varying Capacitance

    Follow-up: How do you increase the charge?

    Since , when the spacing d is doubled, the

    capacitance C is halved.

    And since , that means the

    charge must decrease.

    Q =CΞ”V

    400 V

    π‘ͺ β‰π‘ΈπœŸπ‘½π‘ͺ

    π‘ͺπœΊπŸŽπ‘¨π’…

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Parallel-plate capacitor

    We can increase capacitance by increasing area A by making β€œa roll of metal and insulator”

    π‘ͺπœΊπŸŽπ‘¨π’…

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Parallel-plate capacitor/keyboard

    The keys on most computer keyboards are capacitor switches. Pressing the key pushes two capacitor plates closer together, increasing their capacitance.

    I didn’t know that!

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Combinations of Capacitors

    In practice, two or more capacitors are sometimes connected together.The circuit diagrams below illustrate two basic combinations:

    parallel capacitors and series capacitors.

    The equivalent capacitance is the capacitance of the single capacitor that can replace a set of connected capacitors

    without changing the operation of the circuit

    Wake me up on Friday!

    A method of an equivalent capacitor

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Capacitors in ParallelConsider three capacitors connected in parallel.

    Q

    Real

    circ

    uit

    Equi

    vale

    nt c

    ircui

    t

    Ξ”V

    , Ξ”V

    , Ξ”V

    , Ξ”V

    Q Ξ”V

    Ceq

    Capacitorsinparallelhavethesamepotentialdifference,Ξ”V

    Q is a total charge drawn from the battery 𝑸 π‘ΈπŸ+π‘ΈπŸ+π‘ΈπŸ‘

    Since

    𝑸 π‘ͺπ’†π’’πš«π‘½

    π‘ͺ β‰π‘ΈπœŸπ‘½

    π‘ΈπŸ π‘ͺπŸπœŸπ‘½;π‘ΈπŸ π‘ͺπŸπœŸπ‘½;π‘ΈπŸ‘ π‘ͺπŸ‘πœŸπ‘½;

    We have replaced 3 capacitors with a β€œequivalent” capacitor.

    π‘ͺπ’†π’’πš«π‘½ π‘ͺπŸπš«π‘½+π‘ͺπŸπš«π‘½+π‘ͺπŸ‘πš«π‘½

    π‘ͺ π‘ͺ𝟏+π‘ͺ𝟐+π‘ͺπŸ‘

    Conservation of charge

    Ceq is inserted without changing the operation of the circuit, so Q and Ξ”V are same as in the real circuit

    Equivalentcapacitanceofcapacitorsinparallel.

    πœŸπ‘½ πœŸπ‘½πŸ πœŸπ‘½πŸ = πœŸπ‘½πŸ‘ = πœŸπ‘½π’†π’’

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    𝟏π‘ͺ𝒆𝒒

    𝟏π‘ͺ𝟏

    𝟏π‘ͺ𝟐

    𝟏π‘ͺπŸ‘

    𝑸π‘ͺ𝒆𝒒

    𝑸π‘ͺ𝟏

    + 𝑸π‘ͺ𝟐

    + 𝑸π‘ͺπŸ‘

    Capacitors in SeriesConsider three capacitors connected in series.

    QRea

    l circ

    uit

    Equi

    vale

    nt c

    ircui

    t

    +Q

    Q

    Ξ”V

    Ceq

    Capacitorsinserieshavethesamecharge,Q.

    πœŸπ‘½ πœŸπ‘½πŸ+πœŸπ‘½πŸ+πœŸπ‘½πŸ‘

    Since π‘ͺ β‰π‘ΈπœŸπ‘½

    Ceq is inserted without changing the operation of the circuit, so Q and Ξ”V are same as in the real circuit

    Equivalentcapacitanceofcapacitorsinseries.

    C1 C2 C3

    + -

    -Q +Q -Q +Q -Q

    Ξ”V

    Ξ”V1 Ξ”V2 Ξ”V3

    𝐐 π‘ΈπŸ π‘ΈπŸ π‘ΈπŸ‘

    πœŸπ‘½πŸπ‘Έπ‘ͺ𝟏

    πœŸπ‘½πŸπ‘Έπ‘ͺ𝟐

    πœŸπ‘½πŸ‘π‘Έπ‘ͺπŸ‘

    πš«π‘½ 𝑸 π‘ͺ𝒆𝒒

    Qeq

  • Once the battery is disconnected, Q has to remain constant,

    since no charge can flow either to or from the battery.

    A parallel-plate capacitor initially has apotential difference of 400 V and is thendisconnected from the charging battery. If theplate spacing is now doubled, what is the newvalue of the voltage?

    A) 100 V

    B) 200 V

    C) 400 V

    D) 800 V

    E) 1600 V

    +Q –Q

    ConcepTest Varying Capacitance

    Since , when the spacing d is doubled, the

    capacitance C is halved.

    And since , that means the

    voltage must double.

    400 VQ =CΞ”Vπ‘ͺ β‰π‘ΈπœŸπ‘½π‘ͺ

    π‘ͺπœΊπŸŽπ‘¨π’…

    End of Class

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Example Equivalent capacitance

  • PHYS.1440 Lecture 11 A.DanylovDepartment of Physics and Applied Physics

    Thank you