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Electrostatics and Fields

Electromagnetism explains how charges create fields and forces. This chapter builds the vocabulary of fields, charges, Coulomb's law and Gauss's law.
What you will learn: 1. Scalar and vector fields, field lines, divergence and flux. 2. Charge, Coulomb's law and continuous charge distributions. 3. The electric field and Gauss's law.

Vector and Scalar Fields

A field assigns a quantity to every point in space, and flux and divergence describe how a vector field flows.
A scalar field assigns a number to each point (temperature). A vector field assigns a vector (electric field, fluid velocity). Field lines are drawn tangent to the field, and their density shows its strength. Flux: the flux of a vector field through a surface is the surface integral of the field component normal to the surface, and measures the amount of field crossing it. Divergence: the flux per unit volume leaving an infinitesimal point. Positive divergence marks a source, negative a sink, and zero means no source. The divergence theorem links the flux out of a closed surface to the integral of the divergence inside. Medical relevance: electromagnetic waves are used in MRI, radiofrequency ablation, hyperthermia and tracking systems.

Charge and Coulomb's Law

Charge is quantised and conserved, and the force between point charges falls with the square of the distance.
Charge comes in integer multiples of the elementary charge e = 1.6 x 10^-19 C and is conserved. Like charges repel and opposite charges attract. Coulomb's law: F = k q1 q2 / r^2, with k = 1/(4 pi epsilon0) about 9 x 10^9 N m^2/C^2. The force is along the line joining the charges. For several charges, forces add as vectors (superposition). Continuous distributions: charge is described by a density: volume density rho (C/m^3), surface density sigma (C/m^2) and linear density lambda (C/m). Total charge is the integral of the density.

Electric Field and Gauss's Law

The electric field is force per unit charge, and Gauss's law relates its flux through a closed surface to the enclosed charge.
Electric field: E = F/q. For a point charge E = k q / r^2 directed away from a positive charge. Gauss's law (integral form): the flux of E through a closed surface equals Q_enclosed / epsilon0. In differential form: divergence of E = rho / epsilon0. Use: for symmetric charge distributions Gauss's law gives E directly (sphere, infinite line, infinite plane). Inside a conductor in electrostatic equilibrium E = 0 and excess charge sits on the surface. Electric potential V: work per unit charge, E = minus gradient of V. Field lines are perpendicular to equipotential surfaces.

Check Yourself: Electrostatics and Fields

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. What does a positive divergence mean? 2. State Coulomb's law. 3. Which charge density describes a charged wire? 4. State Gauss's law in integral and differential forms. 5. What is the field inside a conductor in equilibrium?
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. The point is a source of the field. 2. F = q1 q2 / (4 pi epsilon0 r^2), directed along the line joining the charges. 3. Linear charge density (C/m). 4. Flux of E through a closed surface = Q_enclosed / epsilon0; divergence of E = rho / epsilon0. 5. Zero.

Electric Current and Magnetostatics

Moving charges make currents, and currents make magnetic fields. This chapter covers Ohm's law, conservation of charge and the magnetic field.
What you will learn: 1. Current, current density, Ohm's law and power. 2. Conservation of charge. 3. The magnetic field, Oersted's experiment and magnetic induction.

Electric Current

Current is the flow of charge, and in a conductor it is proportional to the applied field.
Current I is charge crossing a section per unit time (amperes). Current density J = n q v (A/m^2), a vector field; I is the flux of J through the section. Ohm's law: microscopic J = sigma E with conductivity sigma; macroscopic V = R I with R = L/(sigma A). Power dissipated: P = V I = R I^2 (Joule heating), which is the basis of resistive heating and electrosurgery. Conservation of charge: the divergence of J plus the rate of change of charge density is zero (the continuity equation). Semiconductors are doped to add carriers (n or p type).

The Magnetic Field

Moving charges create magnetic fields, and the magnetic field lines always close on themselves.
Magnets have two poles that cannot be isolated. Oersted showed that a current deflects a compass, which links electricity and magnetism. Magnetic induction B (tesla) is defined by the force on a moving charge: F = q v x B (Lorentz force). Magnetic field lines are closed loops, so divergence of B = 0 (no magnetic monopoles). Ampere's law: the circulation of B around a closed path equals mu0 times the enclosed current. A long straight wire gives B = mu0 I / (2 pi r); the field inside a long solenoid is mu0 n I. Materials: paramagnetic, diamagnetic and ferromagnetic. Clinical tip: MRI magnets are 1.5-3 T, tens of thousands of times Earth's field.

Check Yourself: Electric Current and Magnetostatics

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. Write the microscopic form of Ohm's law. 2. What is the continuity equation? 3. Why are magnetic field lines closed? 4. Give the field of a long solenoid.
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. J = sigma E. 2. Divergence of J plus d(rho)/dt equals zero: charge is conserved. 3. There are no magnetic monopoles, so divergence of B is zero. 4. B = mu0 n I.

Electromagnetic Induction and Maxwell's Equations

Changing magnetic fields create electric fields. This is the principle of generators, transformers and the wireless transfer of energy, and it completes Maxwell's equations.
What you will learn: 1. Faraday's and Lenz's laws. 2. The full set of Maxwell's equations.

Faraday's and Lenz's Laws

A changing magnetic flux induces an electromotive force, and its direction opposes the change.
Faraday's law: the emf around a closed loop equals minus the rate of change of magnetic flux through it: emf = -d(Phi)/dt. Differential form: curl E = -dB/dt. Lenz's law: the induced current creates a field that opposes the change in flux (the minus sign; conservation of energy). Applications: generators, transformers, inductors, induction heating, eddy currents. Medical: MRI gradients induce currents in tissue (peripheral nerve stimulation limits), and pickup coils detect the MRI signal.

Maxwell's Equations

Together with the Lorentz force, Maxwell's four equations describe all classical electromagnetism and predict electromagnetic waves.
1. Gauss (electric): divergence of E = rho/epsilon0. 2. Gauss (magnetic): divergence of B = 0. 3. Faraday: curl E = -dB/dt. 4. Ampere-Maxwell: curl B = mu0 J + mu0 epsilon0 dE/dt. Maxwell added the displacement current term (dE/dt) so that a changing electric field also creates a magnetic field. This makes possible self-sustaining electromagnetic waves travelling at c = 1/sqrt(mu0 epsilon0), about 3 x 10^8 m/s.

Check Yourself: Electromagnetic Induction and Maxwell's Equations

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. State Faraday's law. 2. What does Lenz's law say? 3. Which term did Maxwell add to Ampere's law and why?
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. emf = -d(flux)/dt. 2. The induced current opposes the change of flux that causes it. 3. The displacement current, so that changing electric fields produce magnetic fields and to keep charge conserved; it predicts electromagnetic waves.

Transmission Lines and Electromagnetic Waves

Signals travel along cables and through space as waves. This chapter describes waves on transmission lines and plane electromagnetic waves in media.
What you will learn: 1. Transmission line theory. 2. Plane waves, propagation in media, reflection and transmission.

Transmission Lines

When the wavelength is comparable to the length of the line, it must be described by distributed inductance and capacitance.
A transmission line is modelled by series inductance and resistance and shunt capacitance and conductance per unit length. The telegraphist equations link voltage and current along the line and give wave solutions: forward and backward travelling waves in phasor form. Lossless line: characteristic impedance Z0 = sqrt(L/C) and propagation velocity 1/sqrt(LC). The reflection coefficient at a load ZL is (ZL - Z0)/(ZL + Z0); with a matched load there is no reflection. A mismatch creates standing waves, characterised by the standing wave ratio. Medical relevance: coaxial cables and microwave circuits connecting antennas and applicators.

Electromagnetic Waves in Media

A plane wave has perpendicular electric and magnetic fields and propagates with a speed and attenuation determined by the medium.
In free space a plane wave has E and B perpendicular to each other and to the direction of propagation, in phase, with |E| = c |B|. Frequency f, wavelength lambda and speed satisfy c = f lambda. In a medium the speed is v = 1/sqrt(mu epsilon) and the wave is attenuated in lossy materials such as tissue (finite conductivity). Penetration (skin) depth decreases with frequency. At a boundary between two media part of the wave is reflected and part transmitted (Fresnel coefficients); at normal incidence the problem is equivalent to a transmission line problem, with wave impedances in place of characteristic impedances.

Check Yourself: Transmission Lines and Electromagnetic Waves

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. What are the two travelling waves on a transmission line? 2. When is there no reflection at the load? 3. How does penetration depth in tissue vary with frequency?
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. A forward wave (towards the load) and a backward (reflected) wave. 2. When the load impedance equals the characteristic impedance. 3. It decreases as frequency increases.

Antennas, Radar and Optical Propagation

Antennas radiate electromagnetic energy, radar uses it to detect objects, and optical fibres and lasers guide light for medical uses.
What you will learn: 1. Radiation and antenna parameters. 2. Radar principle. 3. Optical sources and fibres.

Radiation and Antennas

An accelerating charge radiates, and antennas are characterised by their radiation pattern, directivity and gain.
The simplest antenna is the Hertzian (short) dipole: a short current element that produces near fields that decay quickly and a far field that decays as 1/r and carries power away. Parameters: radiation pattern (angular distribution of power), directivity (peak intensity relative to an isotropic radiator), gain (directivity times efficiency), bandwidth and polarisation. Two antennas in free space are related by the Friis transmission formula. Biomedical uses: antennas for hyperthermia, wireless implants, body-area networks and tracking systems.

Radar

Radar measures the delay and strength of a reflected pulse to find range and direction of a target.
Radar (radio detection and ranging) sends a pulse and detects the echo. Range = c t / 2, where t is the round-trip delay. Angular resolution depends on the antenna beamwidth. The radar equation links received power to transmitted power, antenna gain, wavelength, and radar cross-section of the target, and falls with the fourth power of distance. History: the Chain Home system and the cavity magnetron. Medical applications: contactless monitoring of breathing and heartbeat and movement detection.

Optical Propagation

Optical fibres guide light by total internal reflection, and lasers produce coherent, monochromatic light.
Optical sources: LEDs and lasers (coherent, narrow spectrum, directional; light amplification by stimulated emission). Dielectric guide: light in a high-index core surrounded by a lower-index cladding is confined by total internal reflection when the angle exceeds the critical angle sin(theta_c) = n2/n1. Modes, dispersion and attenuation limit bandwidth and length. Advantages of fibre: large bandwidth, low loss, immunity to electromagnetic interference, small size. Medical uses: endoscopy, laser surgery and photodynamic therapy.

Check Yourself: Antennas, Radar and Optical Propagation

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. Define directivity and gain of an antenna. 2. How is range obtained in radar? 3. What condition gives total internal reflection in a fibre?
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. Directivity: peak radiation intensity relative to an isotropic source. Gain: directivity multiplied by efficiency. 2. From the round-trip time delay: range = c t / 2. 3. The angle of incidence at the core-cladding interface must exceed the critical angle, requiring core index greater than cladding index.

Medical Applications of Electromagnetic Fields

The interaction of fields with the human body is the basis of imaging and therapy, and also a safety issue.
What you will learn: 1. Nuclear magnetic resonance and MRI. 2. Interaction with tissue, SAR and hyperthermia. 3. Lasers in medicine. 4. Electromagnetic compatibility of medical devices.

Magnetic Resonance

Nuclei with spin precess in a magnetic field at the Larmor frequency, and relaxation times give the tissue contrast used in MRI.
Nuclei with spin (mainly hydrogen) have a magnetic moment. In a static field B0 they precess at the Larmor frequency f = gamma B0 / (2 pi); for hydrogen gamma/(2 pi) is 42.58 MHz/T. A radiofrequency pulse at the Larmor frequency tilts the magnetisation into the transverse plane; the decaying signal is the free induction decay. Relaxation: T1 (longitudinal recovery, spin-lattice) and T2 (transverse decay, spin-spin), different in each tissue, so weighting the sequence gives contrast between fat, water and lesions. The spin echo removes the effect of field inhomogeneity. Field homogeneity of B0 is essential. MRI adds gradient fields to encode position.

Interaction with the Body, SAR and Hyperthermia

Tissue has frequency-dependent conductivity and permittivity, and absorbed energy heats it.
Electromagnetic description of tissue: conductivity and permittivity depend on tissue type (high for muscle, low for fat and bone) and frequency, so tissue absorbs and attenuates waves. SAR (specific absorption rate): power absorbed per unit mass (W/kg), SAR = sigma E^2 / (2 rho) for peak field. Safety limits are set for whole-body and local exposure to avoid excessive heating. Hyperthermia raises tumour temperature to about 41-45 degrees Celsius. Applicators: capacitive RF, inductive RF, and microwave radiative applicators; phased arrays focus the energy on the target by controlled interference. Radiofrequency ablation uses higher temperatures to destroy tissue locally.

Lasers and Electromagnetic Compatibility

Lasers are classified by hazard, and medical devices must operate without interfering with each other.
Laser classes: class 1 and 2 are safe or safe by the blink reflex; class 3 can damage the eye; class 4 can cause skin and eye damage and fire. Medical uses: CO2 laser for skin resurfacing and cutting, other lasers for ablation and coagulation of targeted tissue. Electromagnetic compatibility (EMC) is the ability of a device to function in its environment without disturbing others. In hospitals the main dangers are radiated and conducted interference, electrostatic discharge and surges. Devices must pass EMC tests, but passing does not guarantee safety in every place of use. Simple mitigation includes distance from sources, shielding and proper cabling.

Check Yourself: Medical Applications of Electromagnetic Fields

Try every question before opening the answers. Retrieval, not rereading, is what fixes knowledge in memory.
1. Give the Larmor frequency formula. 2. What are T1 and T2? 3. Define SAR. 4. What is the purpose of a phased array in hyperthermia? 5. What does EMC mean?
Check only after trying. Reread any section where you were wrong and retry tomorrow.
1. f = gamma B0 / (2 pi). 2. T1: longitudinal (spin-lattice) recovery time. T2: transverse (spin-spin) decay time. 3. Specific absorption rate: electromagnetic power absorbed per unit mass of tissue (W/kg). 4. To focus energy on the tumour by interference while sparing surrounding tissue. 5. Electromagnetic compatibility: functioning correctly in an electromagnetic environment without causing interference.