Topics
Electric Charges and Fields
- Electric Charge
- Conductors and Insulators
- Basic Properties of Electric Charge
- Coulomb’s Law
- Forces between Multiple Charges
- Electric Field
- Electric Field Due to a System of Charges
- Physical Significance of Electric Field
- Electric Field Lines
- Electric Flux
- Electric Dipole
- Dipole in a Uniform External Field
- Continuous Charge Distribution
- Gauss’s Law
- Application of Gauss' Law
Electrostatics
Current Electricity
Electrostatic Potential and Capacitance
- Electric Potential and Potential Energy
- Electrostatic Potential
- Electric Potential Due to a Point Charge
- Potential Due to an Electric Dipole
- Potential due to a System of Charges
- Equipotential Surfaces
- Relation Between Electric Field and Electrostatic Potential
- Potential Energy of a System of Charges
- Potential Energy of a Single Charge
- Potential Energy of a System of Two Charges in an External Field
- Potential Energy of a Dipole in an External Field
- Electrostatics of Conductors
- Dielectrics and Polarisation
- Capacitors and Capacitance
- The Parallel Plate Capacitor
- Effect of Dielectric on Capacitance
- Combination of Capacitors
- Energy Stored in a Charged Capacitor
Magnetic Effects of Current and Magnetism
Current Electricity
- Electric Current
- Electric Currents in Conductors
- Ohm's Law
- Drift of Electrons and the Origin of Resistivity
- Mobility of Electrons
- Limitations of Ohm’s Law
- Resistivity of Various Materials
- Temperature Dependence of Resistivity
- Electrical Energy and Power in Conductors
- Cells, EMF, and Internal Resistance
- Cells in Series and in Parallel
- Kirchhoff’s Laws
- Wheatstone Bridge
Electromagnetic Induction and Alternating Currents
Moving Charges and Magnetism
- Electromagnetism
- Magnetic force
- Motion in a Magnetic Field
- Magnetic Field Due to a Current-carrying Conductor: Biot-savart's Law
- Applications of Biot-Savart's Law > Magnetic Field at the Axis of a Circular Current-carrying Loop
- Ampere’s Circuital Law
- Solenoid
- Force Between Two Parallel Currents (Ampere’s Law)
- Torque on a Rectangular Current Loop in a Uniform Magnetic Field
- Circular Current Loop as a Magnetic Dipole
- Moving Coil Galvanometer
- Kirchhoff’s Laws
Electromagnetic Waves
Magnetism and Matter
Electromagnetic Induction
Optics
Dual Nature of Radiation and Matter
Alternating Current
Atoms and Nuclei
Electromagnetic Waves
Electronic Devices
Ray Optics and Optical Instruments
- Ray Optics Or Geometrical Optics
- Reflection of Light by Spherical Mirrors
- Sign Convention for Reflection by Spherical Mirrors
- Focal Length of Spherical Mirrors
- Mirror Equation of Spherical Mirrors
- Refraction of Light
- Total Internal Reflection
- Applications of Total Internal Reflection
- Refraction at a Spherical Surfaces
- Refraction by a Lens
- Power of a Lens
- Combined Focal Length of Two Thin Lenses in Contact
- Refraction of Light Through a Prism
- Optical Instruments
- Microscope and it’s types
- Telescope
Wave Optics
- Concept of Wave Optics
- Huygens Principle
- Refraction of a Plane Wave
- Refraction at a Rarer Medium
- Reflection of a Plane Wave by a Plane Surface
- Coherent and Incoherent Addition of Waves
- Interference of Light Waves and Young’s Experiment
- Diffraction of Light
- The Single Slit
- Seeing the Single Slit Diffraction Pattern
- Polarisation of Light
Communication Systems
The Special Theory of Relativity
Dual Nature of Radiation and Matter
- Understanding Dual Nature of Radiation and Matter
- Electron Emission
- Photoelectric Effect - Hertz’s Observations
- Photoelectric Effect - Hallwachs’ and Lenard’s Observations
- Experimental Study of Photoelectric Effect
- Effects of Intensity and Frequency on Photocurrent
- Photoelectric Effect and Wave Theory of Light
- Einstein’s Photoelectric Equation: Energy Quantum of Radiation
- Particle Nature of Light: The Photon
- Wave Nature of Matter
Atoms
Nuclei
Semiconductor Electronics - Materials, Devices and Simple Circuits
Communication Systems
- Detection of Amplitude Modulated Wave
- Production of Amplitude Modulated Wave
- Basic Terminology Used in Electronic Communication Systems
- Sinusoidal Waves
- Modulation and Its Necessity
- Amplitude Modulation (AM)
- Need for Modulation and Demodulation
- Satellite Communication
- Propagation of EM Waves
- Bandwidth of Transmission Medium
- Bandwidth of Signals
The Special Theory of Relativity
- The Special Theory of Relativity
- The Principle of Relativity
- Maxwell'S Laws
- Kinematical Consequences
- Dynamics at Large Velocity
- Energy and Momentum
- The Ultimate Speed
- Twin Paradox
Introduction
Gauss’s law for magnetism states that the total magnetic flux through any closed surface is zero. This means that as many magnetic field lines enter a closed surface as leave it, so the net count is zero.
This law reflects a central physical fact: isolated magnetic monopoles have not been observed in nature. Therefore, magnetic field lines do not begin or end at a single point; instead, they form continuous closed loops.
Background Recall
Gauss and the idea of flux
The topic is named after Carl Friedrich Gauss, a major mathematician and physicist whose work influenced several areas of science. In physics, Gauss’s law is used to relate the field passing through a closed surface to the source enclosed by that surface.
Recall from electrostatics
In electrostatics, the net electric flux through a closed surface depends on the net electric charge enclosed by that surface. This is different from magnetism, where the corresponding net magnetic flux through a closed surface is always zero.
Definition: Magnetic flux
Magnetic flux is the measure of the magnetic field passing through a surface. It depends on the magnetic field, the area of the surface, and the orientation of the surface.
Definition: Gaussian surface
A Gaussian surface is an imaginary closed surface used to analyse field flux. It may be spherical, cylindrical, cubical, or irregular in shape, but Gauss’s law for magnetism remains valid for every closed surface.
Law: Gauss’s Law for Magnetism
Gauss’s law for magnetism: The net magnetic flux through any closed surface is zero.
Mathematical form
For a closed surface,
This expression means that the total magnetic flux entering and leaving a closed surface balances exactly.
Physical meaning
- Magnetic field lines form closed loops.
- No isolated north pole or isolated south pole has been observed.
- A closed surface cannot enclose a net magnetic “charge” in the way it can enclose electric charge.
- Therefore, total outward magnetic flux is always zero.
Net Flux Is Zero
Imagine a closed balloon-like surface placed anywhere in a magnetic field. If some magnetic field lines enter the surface, they must also leave it because magnetic field lines are continuous loops rather than open-ended lines.
A useful analogy is a looped thread passing through a ring-shaped frame: whenever the thread goes in, it must come out somewhere else. That is why the net magnetic flux through a closed surface is zero.
Example
(a) Do magnetic field lines show force direction on a moving charge?
- Answer: No.
- Reason (simple): Magnetic field lines show how a tiny compass needle aligns, not how a moving charge is pushed. Force on a moving charge is perpendicular to the magnetic field, not along it.
(b) If magnetic monopoles existed, how would Gauss’s law change?
- Current law: Net magnetic flux through any closed surface is zero.
- If monopoles existed: Net flux through a closed surface would equal μ₀ × (magnetic charge enclosed), like Gauss’s law in electrostatics, where flux equals charge divided by ε₀.
(c) Can a bar magnet or a current element act on itself?
- Bar magnet on itself: No torque on itself due to its own field.
- Wire element on itself: No force of an element on itself, but different elements of the same wire can exert forces on each other (for a straight wire, the net internal force is zero).
(d) Can a system with zero net charge still have magnetic moment?
- Answer: Yes.
- Reason (simple): Even if total charge is zero, charges can be moving in loops. These current loops create magnetic moments. Example: atoms in paramagnetic materials have current loops and magnetic dipole moments, even though the atom as a whole is neutral.


