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 transferofelectrons take place.
Example of non conducting bodies are silicon and glass
SIunit 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 - Rateofflow of charge for a particulartime
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 1coulomb of charge flows through an area of cross section in a timeperiodof1second, it is known as 1Ampere.
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
n¹=cations
q¹ is cations charge
n²= cations
q² = 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=W/q
V is volt
W is workdone
q is Electriccharge
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
Vb−Va=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
Conductor L is directly proportional to temp
Semiconductor L is directly proportional to temp
Length of the conductor
L is directly proportional to Resistance
R1/R2=L1/L2
If R¹ and R² are made of the same material
Area of cross section (a)
R is inversely proportional to a
R1/R2=a2/a1
R1/R2=(r2)2/(r1)2
Conductance is the reciprocal of Resistance
G = 1/R
Unit = 1/ ohm
= Ohm -¹
=mho
= Seimen
Resistance of wire of that material of unitlength and unitarea 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.