When a current-carrying solenoid is suspended by a long thread so that it can move freely in the horizontal plane, it comes to rest in the north–south direction. The end of the solenoid other than the one pointing towards the north is called the ‘south pole’.
Topics
Electrostatics
Electric Charges and Fields
- Electric Charge
- Positive and Negative Charges
- Electron Theory of Electrification
- Conductors and Insulators
- Electrostatic Induction
- Important Properties of Electric Charge
- Scalar Form of Coulomb’s Law
- Coulomb's Law in Vector Form
- Principle of Superposition
- Equilibrium of Charge and System of Charges
- Electric Field
- Electric Field Intensity Due to a Point-Charge
- Intensity of Electric Field due to a Continuous Charge Distribution
- Electric Lines of Force
- Electric Dipole
- Electric Field due to an Electric Dipole
- Torque on a Dipole in a Uniform Electric Field
Current Electricity
Gauss' Theorem
- Gauss’s Law
- Electric Flux
- Gauss' Theorem
- Applications of Gauss' Theorem
- Overview: Gauss' Theorem
Magnetic Effects of Current and Magnetism
Electric Potential
- Electric Potential
- Potential and Potential Difference
- Potential Gradient
- Equipotential Surfaces
- Potential Due to an Electric Dipole
- Electric Potential Energy of an Electric Dipole in an Electrostatic Field
- Overview: Electric Potential
Capacitors and Dielectrics
- Conductors and Insulators
- Capacitance of a Conductor
- Capacitors
- Capacitance of a Capacitor
- Combination of Capacitors
- Energy Stored in a Charged Capacitor
- Dielectrics
- Electric Polarisation of Matter
- Effect of Introducing a Dielectric between the Plates of a Charged Capacitor
- Overview: Capacitors and Dielectrics
Electromagnetic Induction and Alternating Currents
Electric Resistance and Ohm's Law
- Electric Current
- Current Density
- Mechanism of Flow of Charge in Metals
- Transport Properties of Free Electrons
- Mobility of Electrons
- Relation between Drift Velocity of Free Electrons and Electric Current
- Electric Resistance
- Ohm's Law
- Experimental Verification of Ohm’s Law
- Ohmic and Non-ohmic Resistors
- Exceptions to Ohm's Law
- Dynamic Resistance
- Derivation of Ohm's Law
- Specific Resistance or Electrical Resistivity
- Ohm's law in Vector Form
- Resistance and Conductor Dimensions
- Effect of Temperature on Resistivity
- Colour Code of Carbon Resistors
- Combinations of Resistances
- Derivation Using Series and Parallel Connections
- Electric Energy and Power
- Commercial Units of Electricity Consumption
- Overview: Electric Resistance and Ohm's Law
Electromagnetic Waves
DC Circuits and Measurements
- Electric cell
- Electromotive Force (emf)
- Terminal Potential Difference
- Internal Resistance of a Cell
- Relation between E, V, and r
- Combinations of Cells
- Kirchhoff’s Laws
- Wheatstone Bridge
- Rheostat
- Metre Bridge: Slide-Wire Bridge
- Potentiometer
- Overview: DC Circuits and Measurements
Optics (Ray and Wave Optics)
Dual Nature of Radiation and Matter
Moving Charges and Magnetic Field
- Magnetic Field
- Oersted's Experiment
- Biot-Savart Law
- Comparison of Coulomb's Law and Biot-Savart's Law
- Rules to Determine the Direction of Developed Magnetic Field
- Applications of Biot-Savart's Law > Magnetic Field due to a Finite Straight Current-Carrying Wire
- Applications of Biot-Savart's Law > Magnetic Field on the Axis of a Circular Current-Carrying Loop
- Applications of Biot-Savart's Law > Magnetic Field at the Centre of a Circular Loop
- Ampere’s Circuital Law
- Applications of Ampere’s Circuital Law > Magnetic Field of a Long Straight Solenoid
- Applications of Ampere’s Circuital Law > Magnetic Field of a Long Straight Thin Wire
- Applications of Ampere’s Circuital Law > Magnetic Field of a Toroidal Solenoid
- Force on a Moving Charge in a Uniform Magnetic Field
- Magnetic Field Defined by Magnetic Force
- Motion of Charged Particles in a Uniform Magnetic Field
- Lorentz Force
- Cyclotron
- Force on a Current - Carrying Conductor in a Uniform Magnetic Field
- Ampere: Based on Force Between Currents
- Overview: Moving Charges and Magnetic Field
Atoms and Nuclei
Torque on a Current-Loop : Moving-Coil Galvanometer
- Torque on a Current-Loop in a Uniform Magnetic Field
- Magnetic Moment of a Coil
- Moving Coil Galvanometer
- Sensitivity of a Galvanometer
- Conversion of a Galvanometer into an Ammeter
- Conversion of a Galvanometer into a Voltmeter
- Overview: Torque on a Current-Loop : Moving-Coil Galvanometer
Magnetic Field and Earth's Magnetism
- Current Loop as a Magnetic Dipole: Magnetic Dipole Moment of Current Loop
- Magnetic Dipole Moment of a Revolving Electron
- Magnetic Field of a Magnetic Dipole (Small Bar Magnet)
- Torque on a Magnetic Dipole (Bar Magnet) in a Uniform Magnetic Field
- Potential Energy of a Magnet in a Magnetic Field
- Current-Carrying Solenoid as an Equivalent to a Bar Magnet
- Magnetic Lines of Force
- Earth’s Magnetic Field
- Elements of the Earth's Magnetic Field > Angle of Declination
- Elements of the Earth's Magnetic Field > Angle of Dip or Magnetic Inclination
- Elements of the Earth's Magnetic Field > Horizontal Component of Earth's Magnetic Field
- Overview: Magnetic Field and Earth's Magnetism
Electronic Devices
Communication Systems
Magnetic Classification of Substances
- Classification of Substances According to their Magnetic Behaviour
- Terms Used in Magnetism
- Properties of Dia-, Para-, and Ferromagnetic Substances
- Explanation of Dia-, Para-, and Ferromagnetism based on the Atomic Model of Magnetism
- Hysteresis: Retentivity and Coercivity
- Differences in Magnetic Properties of Soft Iron and Steel
- Magnetic Materials
- Overview: Magnetic Classification of Substances
Electromagnetic Induction
- Magnetic Flux
- Electromagnetic Induction
- Faraday's Laws of Electromagnetic Induction
- Induced Current and Induced Charge
- Methods of Changing the Magnetic Flux
- Motion of a Straight Conductor in a Uniform Magnetic Field (Motional EMF)
- Explanation of Electromagnetic Induction in Terms of Lorentz Force: Proof of Faraday's Law
- Motional emf in Rotating a Conducting Rod in a Uniform Magnetic Field
- Self – Induction
- Self-Inductance of a Long Solenoid
- Energy Stored in an Inductor
- Examples of the Effects of Self-Induced Current
- Mutual Induction
- Mutual Inductance
- Eddy Currents or Foucault Currents
- Overview: Electromagnetic Induction
Alternating Current
- Alternating Voltage and Current in a Rotating Coil
- Definitions Regarding Alternating Voltage and Current
- Mean (or Average) Value of Alternating Current (or Voltage)
- Root-Mean-Square Value of Alternating Current
- Phasors and Phasor Diagrams
- Types of AC Circuits
- Circuit containing Resistance Only
- Circuit containing Inductance Only
- Circuit containing Capacitance Only
- Circuit containing Inductance and Resistance in Series (L-R Series Circuit)
- Circuit containing Capacitance and Resistance in Series (C-R Series Circuit)
- Circuit containing Inductance and Capacitance (L-C Circuit)
- Circuit containing Inductance, Capacitance and Resistance in Series (L-C-R Series Circuit)
- Power in AC Circuit
- Wattless Current
- Half Power Points, Bandwidth and Q-Factor
- Choke Coil
- Electrical Oscillations in L-C Circuit
- Resonant Circuits
- Frequency Response of AC Circuits
- A.C. Generator
- Transformers
- Utility of Alternating Current in Comparison to Direct Current
- Overview: Alternating Current
Electromagnetic Waves
- Displacement Current
- Relation between Conduction and Displacement Current
- Maxwell's Equation
- EM Wave
- Field Magnitude Relation in Free Space
- Energy Density in Electromagnetic Waves
- Transverse Nature of Electromagnetic Waves
- Electromagnetic Spectrum
- Overview: Electromagnetic Waves
Reflection of Light: Spherical Mirrors
- Spherical Mirrors
- Fundamental Terms Related to Spherical Mirrors
- Relation Between Focal Length and Radius of Curvature of a Spherical Mirror
- Rules to Trace the Image Formed by Spherical Mirrors
- Conditions of Image Formation
- Position and Nature of Image Formed by Spherical Mirrors
- Sign Convention
- Mirror Formula for Concave Mirror
- Mirror Formula for Convex Mirror
- Linear Magnification by Spherical Mirrors
- Uses of Spherical Mirrors
- Overview: Reflection of Light: Spherical Mirrors
Refraction of Light at a Plane Interface : Total Internal Reflection : Optical Fibre
- Refraction of Light
- Laws of Refraction
- Cause of Refraction
- Physical Significance of Refractive Index
- Reversibility of Light
- Refraction of Light Through a Rectangular Glass Block
- Refraction through Parallel Multiple Media
- Real and Apparent Depths: Normal Displacement
- Critical Angle
- Total Internal Reflection
- Applications of Total Internal Reflection
- Overview: Refraction of Light at a Plane Interface
Refraction of Light at Spherical Surfaces : Lenses
- Coordinate Geometry Sign Convention for Measuring Distances and Lengths
- Refraction at Concave Spherical Surface
- Refraction at a Convex Spherical Surface
- Concept of Lenses
- Converging and Diverging Actions of Lenses
- Lens Maker's Formula
- Factors Affecting Focal Length of a Lens
- Image Formation by Thin Lenses
- Ray Diagrams for Formation of Image by a Convex Lens
- Ray Diagram for Formation of Image by a Concave Lens
- Linear Magnification by Spherical Lenses
- Power of a Lens
- Combined Focal Length of Two Thin Lenses in Contact
- Combination of Lenses and Mirrors
- Overview: Refraction of Light at Spherical Surfaces: Lenses
Refraction and Dispersion of Light through a Prism
Optical Instruments
Wave Nature of Light : Huygens' Principle
Interference of Light
Diffraction of Light
Polarisation of Light
Photoelectric Effect
Matter Waves
X-Rays
Atom, Origin of Spectra : Bohr's Theory of Hydrogen Atom
Nuclear Structure
Radioactivity
Mass-Energy Equivalence : Nuclear Binding Energy
Nuclear Fission and Nuclear Fusion : Sources of Energy
Semiconductor Electronics
Junction Diodes
Junction Transistors
Logic Gates
Communication Systems
CISCE: Class 12
Definition: Gyromagnetic Ratio
The ratio of the magnitude of the magnetic dipole moment to the magnitude of the angular momentum of the revolving electron is a constant, independent of the details of the orbit. This ratio is called the ‘gyromagnetic ratio’ for the electron.
CISCE: Class 12
Definition: Bohr Magneton
The minimum value of the magnetic dipole moment of an electron is called the Bohr magneton. 1 Bohr-magneton = 9.27 × 10-24 A-m².
CISCE: Class 12
Definition: North Pole
When a current-carrying solenoid is suspended by a long thread so that it can move freely in the horizontal plane, then it always rests in the north-south direction. The end of the solenoid pointing north is called the ‘north pole'.
CISCE: Class 12
Definition: South Pole
CISCE: Class 12
Definition: Magnetic Lines of Force
The lines of force in a magnetic field are those imaginary lines which continuously represent the direction of the magnetic field. The tangent drawn at any point on a line of force shows the direction of magnetic field at that point.
CISCE: Class 12
Definition: Geomagnetic Poles of the Earth
The two places where the needle becomes perpendicular to the Earth’s surface, that is, vertical, are called the geomagnetic poles of the Earth.
CISCE: Class 12
Definition: Magnetic Axis
The line joining the magnetic north and the magnetic south poles of the earth is called the 'magnetic axis' of earth.
CISCE: Class 12
Definition: Magnetic Equator
The plane perpendicular to the magnetic axis of the earth and passing through the points where the magnetic needle is parallel to the earth's surface intersects the earth’s spherical surface into a circle. This 'circle' is called the 'magnetic equator' of the earth.
CISCE: Class 12
Definition: Angle of Declination
At any place, the acute angle between the magnetic meridian and the geographical meridian is called the 'angle of declination'.
CISCE: Class 12
Definition: Angle of Dip or Magnetic Inclination
The angle of dip at a place is the angle between the direction of earth's magnetic field and the horizontal in the magnetic meridian at that placе.
CISCE: Class 12
Definition: Horizontal Component of Earth's Magnetic Field
The horizontal component is the component of the earth’s magnetic field in the horizontal direction in the magnetic meridian.
CISCE: Class 12
Formula: Magnetic Field on the Axial Line of a Dipole
B = \[\frac{\mu_{0}}{4\pi}\frac{2m}{r^{3}}\]
CISCE: Class 12
Formula: Magnetic Field on Equatorial Line of Dipole
B = \[\frac{\mu_0}{4\pi}\frac{m}{r^3}\]
CISCE: Class 12
Formula: Angle of Dip
\[\theta=\tan^{-1}\left(\frac{B_{V}}{B_{H}}\right)\]
CISCE: Class 12
Key Points: Magnetic Dipole of a Current Loop
- A current-carrying loop behaves like a magnetic dipole, similar to a bar magnet.
- When placed in a uniform magnetic field, a current loop experiences a torque that tends to align its axis parallel to the field.
- By comparing the torque on a current loop with that on an electric dipole, the magnetic dipole moment of a current loop is defined as m = I A.
- The direction of the magnetic dipole moment is perpendicular to the plane of the loop and is given by the right-hand curled-finger rule.
- For a coil having N turns, the magnetic dipole moment is
m = N I A, and its SI unit is A·m².
CISCE: Class 12
Key Points: Magnetic Dipole Moment of a Revolving Electron
- An electron revolving around the nucleus behaves like a tiny current loop and hence acts as a magnetic dipole.
- The magnetic dipole moment of a revolving electron arises due to its orbital motion and is perpendicular to the plane of the orbit.
- The direction of magnetic dipole moment is opposite to the direction of the electron’s orbital angular momentum.
CISCE: Class 12
Key Points: Magnetic Torque on a Dipole
- A bar magnet placed in a uniform magnetic field experiences a torque that tends to align its magnetic axis parallel to the field.
- A current loop behaves like a magnetic dipole, and its behaviour in a magnetic field is similar to that of a bar magnet.
- According to the modern theory, a magnet consists of many tiny current loops, and the total torque on the magnet is the sum of torques on these loops.
- The torque depends on the magnet's orientation in the magnetic field and is maximum when the magnetic axis is perpendicular to the field.
- When the magnetic axis is parallel or antiparallel to the magnetic field, the torque becomes zero, and the magnet is in equilibrium.
CISCE: Class 12
Key Points: Equivalence of Solenoid and Bar Magnet
- Two current-carrying solenoids show attraction and repulsion; unlike poles attract each other, while like poles repel each other.
- The polarity of a solenoid is determined by the end rule: anti clockwise current at an end indicates a north pole, and clockwise current indicates a south pole.
- The far axial magnetic field of a finite solenoid is
B = \[\frac{\mu_{0}}{4\pi}\frac{2m}{r^{3}}\],
which is the same as the axial magnetic field of a bar magnet, proving their magnetic equivalence.
CISCE: Class 12
Key Points: Properties of Magnetic Lines of Force
- Magnetic lines of force emerge from the north pole, enter the south pole, and return to the north pole, forming closed, continuous loops.
- No two magnetic lines of force ever intersect, because intersection would imply more than one direction of the magnetic field at a point, which is impossible.
- The density of magnetic lines of force represents field strength; lines are closer near the poles, where the field is strong, and farther apart where the field is weak.
- In a uniform magnetic field, such as the Earth’s magnetic field at a place, the lines of force are parallel and equally spaced.
- Magnetic lines of force do not pass through a neutral point and may enter or leave a magnetic pole at any angle.
