Book contents
- Frontmatter
- Contents
- Introduction
- The Tautological Toolkit
- Rise and Fall: The Logistic Equation
- Mechanics and Gravity: Newton’s Dynamical Equations and Universal Law of Gravity
- The Electromagnetic Force: The Lorentz Force Law
- A Local Conservation Law: The Continuity Equation
- Electrodynamics: The Maxwell Equations
- Electromagnetic Waves: The Wave Equations
- Solitary Waves: The Korteweg–De Vries Equation
- Thermodynamics: The Three Laws of Thermodynamics
- Kinetic Theory: The Boltzmann Equation
- Hydrodynamics: The Navier–Stokes Equations
- Special Relativity: Relativistic Kinematics
- General Relativity: the Einstein Equations
- Quantum Mechanics: the Schrödinger Equation
- The Relativistic Electron: the Dirac Equation
- The Strong Force: Quantum Chromodynamics
- Electro-Weak Interactions: The Glashow–Weinberg–Salam Model
- String Theory: The Superstring Action
- Back To the Future: A Final Perspective
The Electromagnetic Force: The Lorentz Force Law
Published online by Cambridge University Press: 09 February 2021
- Frontmatter
- Contents
- Introduction
- The Tautological Toolkit
- Rise and Fall: The Logistic Equation
- Mechanics and Gravity: Newton’s Dynamical Equations and Universal Law of Gravity
- The Electromagnetic Force: The Lorentz Force Law
- A Local Conservation Law: The Continuity Equation
- Electrodynamics: The Maxwell Equations
- Electromagnetic Waves: The Wave Equations
- Solitary Waves: The Korteweg–De Vries Equation
- Thermodynamics: The Three Laws of Thermodynamics
- Kinetic Theory: The Boltzmann Equation
- Hydrodynamics: The Navier–Stokes Equations
- Special Relativity: Relativistic Kinematics
- General Relativity: the Einstein Equations
- Quantum Mechanics: the Schrödinger Equation
- The Relativistic Electron: the Dirac Equation
- The Strong Force: Quantum Chromodynamics
- Electro-Weak Interactions: The Glashow–Weinberg–Salam Model
- String Theory: The Superstring Action
- Back To the Future: A Final Perspective
Summary
Newton's dynamical equations hold for any force that may 28 be applied to an object. Newton himself gave the expression for the gravitational force. Of the other forces in nature, the electromagnetic force is of paramount importance, because it is the force that keeps atoms and molecules together. To a large extent this force is responsible for the properties of ordinary matter in all its diverse manifestations, from solids to nerve cells. Basic to all these manifestations is the understanding of the force exerted on a charged particle when it moves through a given external electric and magnetic field. Hendrik Antoon Lorentz established the electromagnetic force law in its general form.
The Lorentz force law contains two contributions. The first term in the equation tells us that an arbitrary (positive) charge q moving in an electric field feels a force in the same direction as the electric field E. This means that if the electric field is uniform in space and constant in time, the force exerted on the charged particle will be constant, and therefore the particle will move with a constant acceleration in the direction of the electric field. A big charge feels a stronger force than a small charge, and will feel a stronger acceleration if it has the same mass. Indeed, electric fields can be used to accelerate particles. This force also leads to the attraction between two oppositely charged particles: the one charge feels the force of the electric field caused by the other, which may result in them forming a bound pair.
Now the second term, describing the force resulting from a magnetic field B, is of a very different nature. Note that the force is again proportional to the charge q, but also to the velocity v of the particle. Maybe surprisingly, this means that a particle at rest does not feel the magnetic field. The ‘cross’ a product of the two vectors v and B means that the force is perpendicular to both the velocity of the charge and the magnetic field, as indicated in the figure. The magnitude of the cross product equals the product of the magnitudes of v and B times the sine of the angle between them. So if the two vectors are parallel, their cross product is zero (because sin 0 = 0).
So what does this magnetic force do?
- Type
- Chapter
- Information
- EquationsIcons of knowledge, pp. 28 - 31Publisher: Amsterdam University PressPrint publication year: 2005