Welcome, students! In this 'Deep Dive' section, we're going to explore Ohm's Law and resistivity with a level of detail and conceptual clarity that will equip you not just for your board exams but also for the challenges of JEE Main & Advanced. We'll start from the fundamental principles and build our way up to the microscopic origins and advanced applications.
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1. Ohm's Law: The Foundation of Current Electricity
At its core, Ohm's Law describes the relationship between voltage, current, and resistance in an electrical circuit.
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1.1 Macroscopic Form: V = IR
You've likely encountered this form:
V = I × R
Where:
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V is the
potential difference (voltage) across the conductor, measured in Volts (V). It represents the "push" or energy per unit charge that drives the current.
*
I is the
current flowing through the conductor, measured in Amperes (A). It's the rate of flow of charge.
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R is the
resistance of the conductor, measured in Ohms (Ω). It's a measure of the opposition to the flow of current.
What does it mean?
Imagine water flowing through a pipe.
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Voltage (V) is like the pressure difference driving the water.
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Current (I) is like the rate of water flow.
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Resistance (R) is like the friction or narrowness of the pipe that restricts the flow.
Ohm's Law states that for a given metallic conductor at a constant temperature, the current flowing through it is directly proportional to the potential difference across its ends.
V ∝ I
This proportionality constant is what we define as Resistance (R).
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1.2 Limitations of Ohm's Law: Ohmic vs. Non-Ohmic Devices
While incredibly useful, Ohm's Law isn't universally applicable. It holds true only for certain materials and conditions.
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Ohmic Devices: These are materials/devices for which the V-I graph is a straight line passing through the origin, indicating that resistance (R = V/I) is constant, independent of the voltage applied or the current flowing. Examples include metallic conductors like copper wire at constant temperature.
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Non-Ohmic Devices: For these, the V-I characteristic is not a straight line, meaning their resistance is not constant. It can change with voltage, current, temperature, or even the direction of current.
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Non-linearity: The relationship between V and I is not linear. E.g., a diode, where current flows predominantly in one direction.
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Dependence on polarity: The magnitude of current changes with the reversal of the potential difference, even if the magnitude of V remains the same. E.g., p-n junction diode.
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Non-unique V-I relationship: For some materials, there might be multiple values of V for a single value of I, or vice-versa. E.g., a gallium arsenide (GaAs) semiconductor exhibits negative resistance region.
JEE Focus: Understanding ohmic and non-ohmic behavior is crucial. Questions often involve interpreting V-I graphs to determine if a component follows Ohm's Law and calculating dynamic resistance (dV/dI) for non-ohmic devices.
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1.3 Microscopic Form of Ohm's Law: J = σE
This is a deeper, more fundamental expression that relates current density to the electric field. It's especially important for JEE Advanced.
Consider a conductor of length L and uniform cross-sectional area A. If a potential difference V is applied across its ends, an electric field E is established within the conductor:
E = V / L
The current flowing through the conductor is I, and we define
current density (J) as the current per unit cross-sectional area:
J = I / A
From the macroscopic Ohm's Law, V = IR. We also know that resistance R can be expressed in terms of resistivity (ρ):
R = ρ (L / A)
Substitute R into Ohm's Law:
V = I × ρ (L / A)
Rearrange this equation:
V / L = (I / A) × ρ
Now, substitute E = V/L and J = I/A:
E = J × ρ
Or, more commonly written using
conductivity (σ), which is the reciprocal of resistivity (σ = 1/ρ):
J = σE
This is the
microscopic form of Ohm's Law. It states that the current density (J) in a material is directly proportional to the electric field (E) applied across it, with the proportionality constant being the conductivity (σ) of the material.
Units: J in A/m², E in V/m, σ in (Ω·m)⁻¹ or Siemens/meter (S/m).
CBSE vs. JEE: While V=IR is sufficient for most CBSE problems, J=σE (and its derivation) is a common topic for JEE and provides a deeper understanding of conduction.
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2. Resistivity (ρ) and Conductivity (σ): Intrinsic Material Properties
While resistance (R) depends on the material, its length, and its cross-sectional area,
resistivity (ρ) is an intrinsic property of the material itself.
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2.1 Definition of Resistivity
For a uniform conductor of length L and cross-sectional area A, its resistance R is given by:
R = ρ (L / A)
From this, we can define resistivity as:
ρ = R (A / L)
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Resistivity (ρ): Measured in Ohm-meters (Ω·m). It quantifies how strongly a given material opposes the flow of electric current. A high resistivity means the material is a poor conductor (like an insulator), while low resistivity means it's a good conductor (like a metal).
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2.2 Conductivity (σ)
Conductivity is simply the reciprocal of resistivity:
σ = 1 / ρ
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Conductivity (σ): Measured in (Ω·m)⁻¹ or Siemens per meter (S/m). It quantifies how well a material conducts electric current.
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2.3 Microscopic Origin of Resistivity (Drift Model)
This is a critical concept for a deep understanding and often tested in JEE. It explains *why* materials resist current flow at a fundamental level.
In a conductor, free electrons move randomly due to thermal energy. When an electric field E is applied, these electrons experience a force (F = -eE) and accelerate in the direction opposite to the field. However, they constantly collide with the fixed positive ions (lattice atoms) in the material. These collisions cause the electrons to lose the kinetic energy gained from the field, leading to a net average velocity in the direction opposite to the field, called the
drift velocity (v_d).
Let's derive the expression for resistivity based on this model:
1.
Force on an electron: F = -eE
2.
Acceleration of an electron: a = F/m = -eE/m (where m is the mass of the electron)
3.
Drift velocity (v_d): In the absence of an electric field, the average velocity is zero. With an electric field, electrons accelerate. Between two successive collisions, an electron accelerates for a time equal to the
relaxation time (τ) (average time between collisions).
So, v_d = aτ = (-eE/m)τ
The magnitude of drift velocity is v_d = eEτ/m.
4.
Relation between current and drift velocity:
If 'n' is the number density of free electrons (number of free electrons per unit volume), 'e' is the charge of an electron, and 'A' is the cross-sectional area of the conductor, then the current I is given by:
I = n A e v_d
5.
Substitute v_d:
I = n A e (eEτ/m)
I = (n e² A τ / m) E
6.
From J = σE:
We know J = I/A. So,
I/A = (n e² τ / m) E
J = (n e² τ / m) E
Comparing this with J = σE, we get the expression for
conductivity (σ):
σ = n e² τ / m
And thus, for
resistivity (ρ):
ρ = 1 / σ = m / (n e² τ)
Where:
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m = mass of an electron
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n = number density of free electrons
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e = charge of an electron
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τ = average relaxation time
This derivation clearly shows that resistivity depends on:
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Number density (n): Higher 'n' means more charge carriers, thus lower ρ (better conductor).
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Relaxation time (τ): Longer 'τ' means fewer collisions, less opposition to flow, thus lower ρ.
JEE Focus: This derivation and the factors influencing ρ are frequently tested. Be prepared to explain how changes in temperature affect 'n' and 'τ' differently for metals and semiconductors.
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2.4 Temperature Dependence of Resistivity
Resistivity is not constant; it changes significantly with temperature.
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For Metals (Conductors):
As temperature increases, the positive ions in the lattice vibrate more vigorously. This increases the frequency of collisions between free electrons and the lattice ions, thereby
decreasing the average relaxation time (τ). Since ρ ∝ 1/τ, the resistivity of metals
increases with temperature.
The number density 'n' for metals is largely independent of temperature.
The relationship is approximately linear over a limited temperature range:
ρT = ρ0 (1 + α(T - T0))
Where:
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ρT = resistivity at temperature T
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ρ0 = resistivity at reference temperature T₀ (often 0°C or 20°C)
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α = temperature coefficient of resistivity. For metals, α is positive. Its unit is °C⁻¹ or K⁻¹.
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For Semiconductors (and Insulators):
As temperature increases, more covalent bonds break, releasing more free electrons and creating holes, thus
significantly increasing the number density of charge carriers (n). Although relaxation time (τ) might decrease due to increased vibrations, the drastic increase in 'n' dominates.
Since ρ ∝ 1/n, the resistivity of semiconductors
decreases with temperature. For these materials, α is negative.
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For Alloys (e.g., Nichrome, Manganin, Constantan):
These materials are designed to have very weak temperature dependence of resistivity. Their α is very small, making them suitable for standard resistors where resistance needs to be stable across temperature changes.
JEE Focus: Problems involving temperature dependence of resistance (using R = R₀(1 + αΔT)) are very common. Remember to use the correct α value and understand its physical implication for different materials.
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3. Resistance vs. Resistivity: A Key Distinction
It's vital to differentiate between these two terms.
Feature |
Resistance (R) |
Resistivity (ρ) |
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Definition |
Opposition to current flow in a specific conductor. |
Intrinsic property of the material quantifying its opposition to current flow. |
Dependence |
Depends on material, length (L), cross-sectional area (A), and temperature. |
Depends only on the material type and temperature (and pressure, to a lesser extent). Independent of L and A. |
Formula |
R = ρ(L/A) |
ρ = R(A/L) or ρ = m/(ne²τ) |
Unit |
Ohm (Ω) |
Ohm-meter (Ω·m) |
Nature |
Extrinsic property (depends on geometry) |
Intrinsic property (material characteristic) |
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4. Solved Examples
Let's apply these concepts with some examples.
Example 1: Calculating Resistance from Resistivity (CBSE/JEE Main Level)
A cylindrical wire of material has a length of 2 m and a diameter of 0.4 mm. If its resistivity is 1.7 × 10⁻⁸ Ω·m, calculate its resistance.
Step-by-step Solution:
1.
Identify given values:
* Length, L = 2 m
* Diameter, d = 0.4 mm = 0.4 × 10⁻³ m
* Resistivity, ρ = 1.7 × 10⁻⁸ Ω·m
2.
Calculate radius (r) and cross-sectional area (A):
* Radius, r = d/2 = (0.4 × 10⁻³ m) / 2 = 0.2 × 10⁻³ m
* Area, A = πr² = π (0.2 × 10⁻³ m)² = π (0.04 × 10⁻⁶ m²) = 4π × 10⁻⁸ m²
3.
Use the formula R = ρ(L/A):
* R = (1.7 × 10⁻⁸ Ω·m) × (2 m) / (4π × 10⁻⁸ m²)
* R = (1.7 × 2) / (4π) Ω
* R = 3.4 / (4 × 3.14159) Ω
* R ≈ 3.4 / 12.566 Ω
*
R ≈ 0.2705 Ω
The resistance of the wire is approximately 0.27 Ω.
Example 2: Temperature Dependence of Resistance (JEE Main Level)
A heating element made of nichrome wire has a resistance of 75.0 Ω at 0°C. If the temperature coefficient of resistivity for nichrome is 1.7 × 10⁻⁴ °C⁻¹, what will be its resistance at 250°C?
Step-by-step Solution:
1.
Identify given values:
* Initial resistance, R₀ = 75.0 Ω (at T₀ = 0°C)
* Temperature coefficient, α = 1.7 × 10⁻⁴ °C⁻¹
* Final temperature, T = 250°C
2.
Calculate the change in temperature (ΔT):
* ΔT = T - T₀ = 250°C - 0°C = 250°C
3.
Use the formula RT = R0(1 + αΔT):
* R
T = 75.0 Ω [1 + (1.7 × 10⁻⁴ °C⁻¹)(250°C)]
* R
T = 75.0 Ω [1 + (1.7 × 250 × 10⁻⁴)]
* R
T = 75.0 Ω [1 + (425 × 10⁻⁴)]
* R
T = 75.0 Ω [1 + 0.0425]
* R
T = 75.0 Ω [1.0425]
*
RT = 78.1875 Ω
The resistance of the heating element at 250°C will be approximately 78.19 Ω.
Example 3: Microscopic Ohm's Law (JEE Advanced Level)
A uniform copper wire of length 5 m and cross-sectional area 1.0 × 10⁻⁶ m² carries a current of 2.5 A. The number density of free electrons in copper is 8.5 × 10²⁸ m⁻³. Calculate the drift velocity of the electrons and the electric field inside the wire. (Given: charge of electron e = 1.6 × 10⁻¹⁹ C, resistivity of copper ρ = 1.7 × 10⁻⁸ Ω·m).
Step-by-step Solution:
1.
Identify given values:
* L = 5 m
* A = 1.0 × 10⁻⁶ m²
* I = 2.5 A
* n = 8.5 × 10²⁸ m⁻³
* e = 1.6 × 10⁻¹⁹ C
* ρ = 1.7 × 10⁻⁸ Ω·m
2.
Calculate drift velocity (v_d) using I = n A e v_d:
* v_d = I / (n A e)
* v_d = 2.5 A / [(8.5 × 10²⁸ m⁻³)(1.0 × 10⁻⁶ m²)(1.6 × 10⁻¹⁹ C)]
* v_d = 2.5 / (8.5 × 1.6 × 10³ m⁻¹)
* v_d = 2.5 / (13.6 × 10³) m/s
* v_d = 0.1838 × 10⁻³ m/s
*
v_d ≈ 1.84 × 10⁻⁴ m/s
3.
Calculate resistance (R) of the wire:
* R = ρ (L / A)
* R = (1.7 × 10⁻⁸ Ω·m) × (5 m) / (1.0 × 10⁻⁶ m²)
* R = (1.7 × 5 × 10⁻²) Ω
* R = 8.5 × 10⁻² Ω = 0.085 Ω
4.
Calculate the potential difference (V) across the wire using Ohm's Law (V=IR):
* V = I × R
* V = 2.5 A × 0.085 Ω
*
V = 0.2125 V
5.
Calculate the electric field (E) inside the wire using E = V/L:
* E = 0.2125 V / 5 m
*
E = 0.0425 V/m
Alternatively, using J = σE:
* Current density, J = I/A = 2.5 A / (1.0 × 10⁻⁶ m²) = 2.5 × 10⁶ A/m²
* Conductivity, σ = 1/ρ = 1 / (1.7 × 10⁻⁸ Ω·m) ≈ 5.88 × 10⁷ (Ω·m)⁻¹
* E = J / σ = (2.5 × 10⁶ A/m²) / (5.88 × 10⁷ (Ω·m)⁻¹)
*
E ≈ 0.0425 V/m (consistent with the previous method)
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By understanding these detailed aspects of Ohm's Law and resistivity, you're now equipped to tackle complex problems in current electricity. Remember to focus on the interplay between macroscopic observations (V, I, R) and their microscopic origins (n, e, τ) for a truly robust conceptual foundation.