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.
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