Current, Resistance, Direct-current Circuits - PowerPoint PPT Presentation

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Current, Resistance, Direct-current Circuits

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Title: Current, Resistance, Direct-current Circuits


1
Current, Resistance, Direct-current Circuits
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  • 1. Electric current
  • The current is the rate at which charge flows
    through this surface
  • Suppose ?Q is the amount of charge that flows
    through an area A in a time interval ?t and that
    the direction of flow is perpendicular to the
    area. Then the current I is equal to the amount
    of charge divided by the time
  • I ? Q/?t
  • SI C/sA
  • (Ampere)

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  • 2. Current and voltage measuraments in circuits

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  • 3. Resistance and Ohms Law
  • Resistance is the ratio of the voltage across the
    conductor to the current
  • R ?V/ I
  • SI units 1V/A1O (Ohms)
  • Ohms Law the resistance remains constant over a
    wide range of applied voltage or currents
  • ?V IR

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  • A resistor is a conductor that provides a
    specified resistance in an electric circuit
  • The resistance is proportional to the conductors
    length l and inversely proportional to its
    cross-sectional area A
  • R ? l/A
  • ? resistivity of the material (ct. of
    proportionality) SI unit O m

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  • 4. Electrical energy and power
  • The rate at which the system loses potential
    energy as the charge passes through resistor is
    equal to the rate at which the system gains
    internal energy in the resistor.
  • (?Q/ ?t) ?V I ?V
  • Power P - the rate at which energy is delivered
    to the resistor
  • P I ?V
  • P I2R ?V2/R
  • SI kilowatt-hour
  • 1kWh (103W)(3600s) 3.6x106J

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  • Question Some homes have light dimmers that are
    operated by rotating a knob. What is being
    changed in the electric circuit when the know is
    rotated?
  • R I

11
Direct-Current Circuits
  • 5. Sources of EMF (electromotive force)- a
    charge pump that forces electrons to move in a
    direction opposite the electrostatic field inside
    the source
  • The emf e of a source is the work done per unit
    charge (SI unit V)
  • ?V e Ir
  • e the terminal voltage when the current is zero
    (open circuit voltage)

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  • ?V IR
  • (R- the external resistance)
  • e IR Ir
  • I e / (Rr)
  • I e I2R I2r if rltltR
  • (the power delivered
  • by the battery is
  • transferred to the load
  • resistance)

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  • 6. Resistors in series

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  • ?V IR1 IR2 I(R1R2)
  • ?V I Req
  • IReq I(R1R2)
  • Req R1R2
  • Req R1R2.
  • The equivalent resistance of a series combination
    of resistors is the algebraic sum of the
    individual resistances and is always greater than
    any individual resistance

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  • 7. Resistors in parallel

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  • The potential differences across resistors are
    the same because each is connected directly
    across the battery terminals
  • Because charge is conserved, the current I that
    enters point a must equal the total current I1I2
    leaving that point
  • I I1I2
  • I1?V /R1
  • I2?V /R2
  • I ?V /Req
  • 1/Req 1/R1 1/R2
  • The inverse of the equivalent resistance of two
    or more resistors connected in parallel is the
    sum of the inverses of the individual resistances
    and is always less than the smallest resistance
    in the group

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  • 8. Kirchhoffs Rules
  • 1. The sum of the currents entering any jonction
    must equal the sum of the currents leaving that
    junction (junction rule)

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  • 2. The sum of the potential differences across
    all the elements around any closed circuit loop
    must be zero (loop rule)

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  • a) if the resistor is traversed in the direction
    of the current, the charge in electric potential
    across the resistor is IR
  • b) If a resistor is traversed in the direction
    opposite the current, the charge in electric
    potential across resistors is IR

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  • c) if a source of emf is traversed in the
    direction of the emf (from to ) the charge in
    electric potential is S
  • d) if a source of emf is traversed in the
    direction opposite the emf, the charge in
    electric potential is -S

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  • Problem solving strategy
  • 1. Assign labels and symbols to all the known and
    unknown quantities
  • 2. Assign directions to the currents in each part
    of the circuit
  • 3. Apply the junction rule to any junction in the
    circuit
  • 4. Apply Kirchhoffs loop rule, to as many loops
    in the circuit as are needed to solve for the
    unknowns
  • 5. solve the equations
  • 6. Check your answers by substituting them into
    the original equations

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  • Problem Find the currents in the circuit shown
    in fig. by using Kirchhoffs rules

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  • 9. RC circuits

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  • We consider that the capacitor is initially
    uncharged with the switch open. After the switch
    is closed, the battery begins to charge the
    plates of capacitor and the charge passes through
    resistor
  • A the capacitor is being charged, the circuit
    carries a changing current. The process continues
    until the capacitor is charged to a maximum value
  • QCe
  • e -maximum voltage across the capacitor
  • Once the capacitor is fully charged, the current
    in circuit is zero

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  • qQ(1-e t/RC)
  • RCs time constant
  • The time constant represents the time required
    for the charge to increase from zero to 63.2 its
    maximum equilibrium value

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  • Before the switch is closed the potential
    difference across the charged capacitor is Q/C
  • Once the switch is closed, the charge begins to
    flow through the resistor, until the capacitor is
    fully charged
  • qQe-t/RC
  • The charge decreasses exponentially with time
  • ?Vee-t/RC

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