Electric Current in Conductors (original) (raw)

Last Updated : 23 Jul, 2025

Electric current in conductors is the movement of electric charge through a substance, usually a metallic wire or other conductor. Electric current is the rate at which an electric charge flows past a certain point in a conductor, and it is measured in amperes.

When a potential difference (voltage) is supplied across the ends of a conductor, it induces an electric field within the material. This electric field exerts force on the free electrons in the conductor, causing them to migrate. In this article, we will learn in detail about the electric current in conductors.

What is Electric Current?

Electric current is defined as the rate at which electric charge flows past a given point in a circuit. It's measured in amperes (A), where 1 ampere is equivalent to 1 coulomb of charge flowing per second.

**Ohm's Law

Ohm's Law describes the relationship between current, voltage, and resistance in a circuit. It states that the current (I) flowing through a conductor is directly proportional to the voltage (V) applied across it and inversely proportional to the resistance (R) of the conductor, expressed by the equation

**I = V/R

In a given time interval "t", the charge passing through the surface can be divided into two parts - positive charges and negative charges. Let's say q+ is the net positive charge passing through the surface in the given time interval, similarly q- is the net negative charge passing through the surface in the given time interval. In this case, the net charge passing through this surface in this interval will be,

**q net = q + - q -

**Electric current in defined as the rate of flow of charge in a conductor.

Here, I represents the average current flowing through the surface.

The unit for current is Ampere (A), Ampere stands for Column/sec.

In case when the rate of flow of charge is varying, the current flowing is given by,

**I = dQ/dt

**Where:

What is Conductors?

Conductors are materials that allow electric current to flow through them easily. In these materials, electric charge carriers, typically electrons, are free to move. Metals like copper, silver, gold, and aluminum are excellent conductors of electricity due to their atomic structure.

In conductors, electrons are loosely bound to their atoms, allowing them to move relatively freely in response to an electric field. When a voltage is applied across a conductor, an electric current is established as electrons drift from areas of higher potential (positive) to areas of lower potential (negative).

Types of Conductors

These are some of the main types of conductors, each with its own unique properties and applications.

Electric Currents in Conductors

An electric charge experiences force if an electric field is applied, due to the force it starts moving and the movement of these charges constitutes the electric current. In a solid conductor, atoms are tightly bound with each other and approximately all the electrons are bound to the atoms. There are some electrons that are free from all the atoms are able to move freely throughout the material. When no electric field is applied, these electrons perform motion in random directions. At a given time, there is no preferential direction for the velocities of the electrons. This means, on average the number of electrons travelling in any direction will be equal to the number of electrons travelling in the opposite direction. So, there will be no net electric current.

Electric Current in Conductor

Let's see how these electrons behave when an electric field is applied to the conductor. Imagine a conductor given in the figure above, suppose one is a positively charges cylindrical disc and a negatively charged cylindrical disc. These discs are kept at the ends of a cylindrical conductor. An electric field will be created inside the conductor, this field will exert the force of charges and they will move. The movement of charges causes the electric current

Direction of Electric Current in Conductor

The direction of electric current in a conductor is defined as the direction in which positive charge carriers would flow if they were free to move. However, in most metallic conductors, such as wires, the charge carriers are negatively charged electrons, which actually move in the opposite direction of conventional current flow.

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Sample Problems on Electric Current in Conductors

**Question 1: Assume a horizontal plate and positive charge of 50C flows in 5 seconds through that plate. Find the magnitude of the electric current passing through that plate.

**Answer:

It is known that electric current is the rate of charge passing through the conductor.

Net charge passing through the conductor qnet = 50C

Time taken, t = 5

I = \frac{q_{net}}{t}

⇒ I = \frac{50}{5}

⇒ I = 10 A

**Question 2: Assume a horizontal plate and positive charge of 20C flows in 2.5 seconds through that plate. Find the magnitude of the electric current passing through that plate.

**Answer:

It is known that electric current is the rate of charge passing through the conductor.

Net charge passing through the conductor qnet = 20C

Time taken, t = 2.5

I = \frac{q_{net}}{t}

⇒ I = \frac{20}{2.5}

⇒ I = 8 A

**Question 3: The charge present inside the conductor at a given time is given by the function q(t) below.

**q(t) = sin(t)

**Find the current flowing through the conductor at time t.

**Answer:

In this case, the rate of charge through the conductor is changing. So, average current cannot be calculated, for such case instantaneous current is calculated.

I = \frac{dq}{dt}

⇒ I = \frac{d(sin(t))}{dt}

⇒ I = cos(t) A

**Question 4: The charge present inside the conductor at a given time is given by the function q(t) below.

**q(t) = t 2 + 2t

**Find the current flowing through the conductor at time t = 2.

**Answer:

In this case, the rate of charge through the conductor is changing. So, average current cannot be calculated, for such case instantaneous current is calculated.

I = \frac{dq}{dt}

⇒ I = \frac{d(t^2 + 2t)}{dt}

⇒ I = \frac{dt^2}{dt} + \frac{2dt}{dt}

⇒ I = 2t + 2

at t = 2.

I = 2(2) + 2

⇒ I = 4 + 2

⇒ I = 6 A

**Question 5: The charge present inside the conductor at a given time is given by the function q(t) below.

**q(t) = t + 2t 3 + e t

**Find the current flowing through the conductor at time t = 1.

**Answer:

In this case, the rate of charge through the conductor is changing. So, average current cannot be calculated, for such case instantaneous current is calculated.

I = \frac{dq}{dt}

⇒ I = \frac{d(t + 2t^3 + e^t)}{dt}

⇒ )I = \frac{d(t)}{dt} + \frac{d(2t^3)}{dt} + \frac{de^t}{dt}

⇒ I = 1 + 6t2 + et

at t = 1.

I = 1 + 6t2 + et

⇒ I = 1 + 6(1) + e

⇒ I = 7 + e

⇒ I = 9.7A