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.