Electricity

Cards (56)

  • When a body loses electrons it is positively charged. When body gains electrons it is negatively charged. This happens in non conducting bodies which are static.
  • When we rub 2 non- conducting bodies transfer of electrons take place.
  • Example of non conducting bodies are silicon and glass
  • SI unit of charge is known as coulomb
  • When charge is lower than 1 coulomb
    • Millicoulomb - 10-³ C
    • Microcoulomb_ 10-⁶ C
    • Nanocoulomb _ 10-⁹ C
  • Charge - scalar quantity
  • Charge of an electron ~ -1.6 × 10-¹⁹ C
  • The quantity of charge is determined by the number of electrons
  • Q = ±ne
    Where n is the no. of electrons and e is charge of an electron
  • n = 6.25 × 10¹⁸ electrons
    i.e 1 coulomb contains 6.25 × 10¹⁸ electrons.
  • Electric current - Rate of flow of charge for a particular time
  • i = q/t
    This is for tiny amount of charge
  • If charge has n no. of electrons,  Total electric current can be written as
    I = Q/ t
    Where Q is the quantity of charge.
  • I = Cs-¹
    Or the SI unit of current is called Ampere
  • When 1 coulomb of charge flows through an area of cross section in a time period of 1 second, it is known as 1 Ampere.
  • Electric current is measured by an Ammeter
  • Electric current is measured by an Ammeter
    Note : Ammeter is always connected in a series circuit
  • Current always flows from high potential to low potential
  • The direction of flow of current is opposite to the direction of motion of electrons
  • In metals only negatively charged electrons move.
    Although in electrolytes and ionised gases both cations and anions move.
    Electrolytes are found in batteries
  • Current moving in electrolytes can be told as
    I = n¹q¹ + n²q²/t
    Where
    =cations
    is cations charge
    = cations
    = anions charge
  • In electrolytes cations and anion move in opposite directions.
  • The work done to bring a unit positive charge from infinity to a point in the electric field is known as Electric potential.
  • Electric potential
    Scalar quantity
  • Electric potential is measured using a voltmeter
  • V=V=W/q W /q
    V is volt
    W is work done
    q is Electric charge
  • Voltmeter is always connected in a parallel circuit
  • Potential difference is the work done to bring a unit positive charge from one point to another within the circuit.
  • SI unit of potential difference is volt
  • VbVa=V_b - V_a =W/q W/q
    Where a and b are the two points I the potential difference.
  • Resistance can be caused be collision of -ve and +ve ions
  • the obstruction given to the flow of charge by the material is known as Resistance.
  • SI unit of resistance is known as Ohm (Ω).
    • Nature of material
    • Temperature
    1. Conductor L is directly proportional to temp
    2. Semiconductor L is directly proportional to temp
    • Length of the conductor
    L is directly proportional to Resistance
    R1/R2=R_1/R_2 =L1/L2 L_1/L_2
    If and are made of the same material
    • Area of cross section (a)
    R is inversely proportional to a
    R1/R2=R_1/R_2 =a2/a1 a_2/a_1
    R1/R2=R_1/R_2 =(r2)2/(r1)2 (r_2)^2/(r_1)^2
  • Conductance is the reciprocal of Resistance
  • G = 1/R
    Unit = 1/ ohm
    = Ohm -¹
    =mho
    = Seimen
  • Resistance of wire of that material of unit length and unit area is known as Specific Resistance
  • Specific resistivity depends on the factors
    • Characteristics / nature of material
    • Temperature
  • R & L (& is directly proportional)
    R& 1/a
    R = p×L/a
    Where p is row and specific resistivity if L and a are 1
  • Difference between Resistance and resistivity
    Resistance is not constant
    Resistivity is constant when L and a are 1 at given temperature.