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The **telegrapher's equations** (or just **telegraph equations**) are a pair of coupled, linear differential equations that describe the voltage and current on an electrical transmission line with distance and time. The equations come from Oliver Heaviside who in the 1880s developed the * transmission line model *. The model demonstrates that the electromagnetic waves can be reflected on the wire, and that wave patterns can appear along the line. The theory applies to transmission lines of all frequencies including high-frequency transmission lines (such as telegraph wires and radio frequency conductors), audio frequency (such as telephone lines), low frequency (such as power lines) and direct current.

In mathematics, a **linear differential equation** is a differential equation that is defined by a linear polynomial in the unknown function and its derivatives, that is an equation of the form

**Voltage**, **electric potential difference**, **electric pressure **or **electric tension** is the difference in electric potential between two points. The difference in electric potential between two points in a static electric field is defined as the work needed per unit of charge to move a test charge between the two points. In the International System of Units, the derived unit for voltage is named *volt*. In SI units, work per unit charge is expressed as joules per coulomb, where 1 volt = 1 joule per 1 coulomb. The official SI definition for *volt* uses power and current, where 1 volt = 1 watt per 1 ampere. This definition is equivalent to the more commonly used 'joules per coulomb'. Voltage or electric potential difference is denoted symbolically by ∆*V*, but more often simply as *V*, for instance in the context of Ohm's or Kirchhoff's circuit laws.

An **electric current** is a flow of electric charge. In electric circuits this charge is often carried by electrons moving through a wire. It can also be carried by ions in an electrolyte, or by both ions and electrons such as in an ionized gas (plasma).

- Distributed components
- Role of different components
- Values of primary parameters for telephone cable
- The equations
- Lossless transmission
- The equations for lossless transmission lines
- Sinusoidal steady-state
- General solution
- Lossy transmission line
- Signal pattern examples
- Solutions of the telegrapher's equations as circuit components
- See also
- Notes
- References

The telegrapher's equations, like all other equations describing electrical phenomena, result from Maxwell's equations. In a more practical approach, one assumes that the conductors are composed of an infinite series of two-port elementary components, each representing an infinitesimally short segment of the transmission line:

**Maxwell's equations** are a set of partial differential equations that, together with the Lorentz force law, form the foundation of classical electromagnetism, classical optics, and electric circuits. The equations provide a mathematical model for electric, optical, and radio technologies, such as power generation, electric motors, wireless communication, lenses, radar etc. Maxwell's equations describe how electric and magnetic fields are generated by charges, currents, and changes of the fields. One important consequence of the equations is that they demonstrate how fluctuating electric and magnetic fields propagate at the speed of light. Known as electromagnetic radiation, these waves may occur at various wavelengths to produce a spectrum from radio waves to γ-rays. The equations are named after the physicist and mathematician James Clerk Maxwell, who between 1861 and 1862 published an early form of the equations that included the Lorentz force law. He also first used the equations to propose that light is an electromagnetic phenomenon.

- The distributed resistance of the conductors is represented by a series resistor (expressed in ohms per unit length).
- The distributed inductance (due to the magnetic field around the wires, self-inductance, etc.) is represented by a series inductor (henries per unit length).
- The capacitance between the two conductors is represented by a shunt capacitor C (farads per unit length).
- The conductance of the dielectric material separating the two conductors is represented by a shunt resistor between the signal wire and the return wire (siemens per unit length). This resistor in the model has a resistance of ohms.

The **electrical resistance** of an object is a measure of its opposition to the flow of electric current. The inverse quantity is **electrical conductance**, and is the ease with which an electric current passes. Electrical resistance shares some conceptual parallels with the notion of mechanical friction. The SI unit of electrical resistance is the ohm (Ω), while electrical conductance is measured in siemens (S).

The **ohm** is the SI derived unit of electrical resistance, named after German physicist Georg Simon Ohm. Although several empirically derived standard units for expressing electrical resistance were developed in connection with early telegraphy practice, the British Association for the Advancement of Science proposed a unit derived from existing units of mass, length and time and of a convenient size for practical work as early as 1861. The definition of the ohm was revised several times. Today, the definition of the ohm is expressed from the quantum Hall effect.

In electromagnetism and electronics, **inductance** describes the tendency of an electrical conductor, such as coil, to oppose a change in the electric current through it. The change in current induces a reverse electromotive force (voltage). When an electric current flows through a conductor, it creates a magnetic field around that conductor. A changing current, in turn, creates a changing magnetic field, the surface integral of which is known as magnetic flux. From Faraday's law of induction, any change in magnetic flux through a circuit induces an electromotive force (voltage) across that circuit, a phenomenon known as electromagnetic induction. Inductance is specifically defined as the ratio between this induced voltage and the rate of change of the current in the circuit

The model consists of an *infinite series* of the infinitesimal elements shown in the figure, and that the values of the components are specified *per unit length* so the picture of the component can be misleading. An alternative notation is to use , , , and to emphasize that the values are derivatives with respect to length. These quantities can also be known as the primary line constants to distinguish from the secondary line constants derived from them, these being the characteristic impedance, the propagation constant, attenuation constant and phase constant. All these constants are constant with respect to time, voltage and current. They may be non-constant functions of frequency.

The **primary line constants** are parameters that describe the characteristics of conductive transmission lines, such as pairs of copper wires, in terms of the physical electrical properties of the line. The primary line constants are only relevant to transmission lines and are to be contrasted with the secondary line constants, which can be derived from them, and are more generally applicable. The secondary line constants can be used, for instance, to compare the characteristics of a waveguide to a copper line, whereas the primary constants have no meaning for a waveguide.

The **characteristic impedance** or **surge impedance** (usually written Z_{0}) of a uniform transmission line is the ratio of the amplitudes of voltage and current of a single wave propagating along the line; that is, a wave travelling in one direction in the absence of reflections in the other direction. Alternatively and equivalently it can be defined as the input impedance of a transmission line when its length is infinite. Characteristic impedance is determined by the geometry and materials of the transmission line and, for a uniform line, is not dependent on its length. The SI unit of characteristic impedance is the ohm.

The **propagation constant** of a sinusoidal electromagnetic wave is a measure of the change undergone by the amplitude and phase of the wave as it propagates in a given direction. The quantity being measured can be the voltage, the current in a circuit, or a field vector such as electric field strength or flux density. The propagation constant itself measures the change per unit length, but it is otherwise dimensionless. In the context of two-port networks and their cascades, **propagation constant **measures the change undergone by the source quantity as it propagates from one port to the next.

The role of the different components can be visualized based on the animation at right.

- The inductance
*L*makes it look like the current has inertia—i.e. with a large inductance, it is difficult to increase or decrease the current flow at any given point. Large inductance makes the wave move more slowly, just as waves travel more slowly down a heavy rope than a light one. Large inductance also increases the wave impedance (lower current for the same voltage). - The capacitance
*C*controls how much the bunched-up electrons within each conductor repel the electrons in the*other*conductor. By absorbing some of these bunched up electrons, the speed of the wave and its strength (voltage) are both reduced. With a larger capacitance, there is less repulsion, because the*other*line (which always has the opposite charge) partly cancels out these repulsive forces*within*each conductor. Larger capacitance equals (weaker restoring force)s making the wave move slightly slower, and also gives the transmission line a lower impedance (higher current for the same voltage). *R*corresponds to resistance within each line, and*G*allows current to flow from one line to the other. The figure at right shows a lossless transmission line, where both*R*and*G*are 0.

**Inertia** is the resistance, of any physical object, to any change in its velocity. This includes changes to the object's speed, or direction of motion.

**Restoring force**, in a physics context, is a force that gives rise to an equilibrium in a physical system. If the system is perturbed away from the equilibrium, the restoring force will tend to bring the system back toward equilibrium. The restoring force is a function only of position of the mass or particle. It is always directed back toward the equilibrium position of the system. The restoring force is often referred to in simple harmonic motion. The force which is responsible to restore original size and shape is called restoring force.

Representative parameter data for 24 gauge telephone polyethylene insulated cable (PIC) at 70 °F (294 K)

Frequency | R | L | G | C | ||||
---|---|---|---|---|---|---|---|---|

Hz | ^{ Ω }⁄_{km} | ^{Ω}⁄_{1000 ft } | ^{ mH }⁄_{km} | ^{mH}⁄_{1000 ft} | ^{ µS }⁄_{km} | ^{µS}⁄_{1000 ft} | ^{ nF }⁄_{km} | ^{nF}⁄_{1000 ft} |

1 Hz | 172.24 | 52.50 | 0.6129 | 0.1868 | 0.000 | 0.000 | 51.57 | 15.72 |

1 kHz | 172.28 | 52.51 | 0.6125 | 0.1867 | 0.072 | 0.022 | 51.57 | 15.72 |

10 kHz | 172.70 | 52.64 | 0.6099 | 0.1859 | 0.531 | 0.162 | 51.57 | 15.72 |

100 kHz | 191.63 | 58.41 | 0.5807 | 0.1770 | 3.327 | 1.197 | 51.57 | 15.72 |

1 MHz | 463.59 | 141.30 | 0.5062 | 0.1543 | 29.111 | 8.873 | 51.57 | 15.72 |

2 MHz | 643.14 | 196.03 | 0.4862 | 0.1482 | 53.205 | 16.217 | 51.57 | 15.72 |

5 MHz | 999.41 | 304.62 | 0.4675 | 0.1425 | 118.074 | 35.989 | 51.57 | 15.72 |

More extensive tables and tables for other gauges, temperatures and types are available in Reeve.^{ [1] } Chen^{ [2] } gives the same data in a parameterized form that he states is usable up to 50 MHz.

The variation of and is mainly due to skin effect and proximity effect.

The constancy of the capacitance is a consequence of intentional, careful design.

The variation of G can be inferred from Terman: “The power factor ... tends to be independent of frequency, since the fraction of energy lost during each cycle ... is substantially independent of the number of cycles per second over wide frequency ranges.”^{ [3] } A function of the form with close to 1.0 would fit Terman’s statement. Chen ^{ [2] } gives an equation of similar form.

G in this table can be modeled well with

Usually the resistive losses grow proportionately to and dielectric losses grow proportionately to with so at a high enough frequency, dielectric losses will exceed resistive losses. In practice, before that point is reached, a transmission line with a better dielectric is used. In long distance rigid coaxial cable, to get very low dielectric losses, the solid dielectric may be replaced by air with plastic spacers at intervals to keep the center conductor on axis.

The telegrapher's equations are:

They can be combined to get two partial differential equations, each with only one dependent variable, either or :

Except for the dependent variable ( or ) the formulas are identical.

When the elements *R* and *G* are very small, their effects can be neglected, and the transmission line is considered as an ideal lossless structure. In this case, the model depends only on the *L* and *C* elements. The Telegrapher's Equations then describe the relationship between the voltage *V* and the current *I* along the transmission line, each of which is a function of position *x* and time *t*:

The equations themselves consist of a pair of coupled, first-order, partial differential equations. The first equation shows that the induced voltage is related to the time rate-of-change of the current through the cable inductance, while the second shows, similarly, that the current drawn by the cable capacitance is related to the time rate-of-change of the voltage.

The Telegrapher's Equations are developed in similar forms in the following references: Kraus,^{ [4] } Hayt,^{ [5] } Marshall,^{ [6] } Sadiku,^{ [7] } Harrington,^{ [8] } Karakash,^{ [9] } and Metzger.^{ [10] }

These equations may be combined to form two exact wave equations, one for voltage *V*, the other for current *I*:

where

is the propagation speed of waves traveling through the transmission line. For transmission lines made of parallel perfect conductors with vacuum between them, this speed is equal to the speed of light.

In the case of sinusoidal steady-state, the voltage and current take the form of single-tone sine waves:

- ,

where is the angular frequency of the steady-state wave. In this case, the Telegrapher's equations reduce to

Likewise, the wave equations reduce to

where *k* is the wave number:

Each of these two equations is in the form of the one-dimensional Helmholtz equation.

In the lossless case, it is possible to show that

and

where is a real quantity that may depend on frequency and is the * characteristic impedance * of the transmission line, which, for a lossless line is given by

and and are arbitrary constants of integration, which are determined by the two boundary conditions (one for each end of the transmission line).

This impedance does not change along the length of the line since *L* and *C* are constant at any point on the line, provided that the cross-sectional geometry of the line remains constant.

The lossless line and distortionless line are discussed in Sadiku,^{ [11] } and Marshall,^{ [12] }

The general solution of the wave equation for the voltage is the sum of a forward traveling wave and a backward traveling wave:

where

- and can be
*any*functions whatsoever, and - is the waveform's propagation speed (also known as phase velocity).

*f*_{1} represents a wave traveling from left to right in a positive x direction whilst *f*_{2} represents a wave traveling from right to left. It can be seen that the instantaneous voltage at any point x on the line is the sum of the voltages due to both waves.

Since the current *I* is related to the voltage *V* by the telegrapher's equations, we can write

When the loss elements *R* and *G* are not negligible, the differential equations describing the elementary segment of line are

By differentiating both equations with respect to *x*, and some algebraic manipulation, we obtain a pair of hyperbolic partial differential equations each involving only one unknown:

Note that these equations resemble the homogeneous wave equation with extra terms in V and I and their first derivatives. These extra terms cause the signal to decay and spread out with time and distance. If the transmission line is only slightly lossy (*R* << ω*L* and *G* << ω*C*), signal strength will decay over distance as *e*^{−αx}, where α ≈ *R*/2*Z*_{0} + *GZ*_{0}/2.^{ [13] }^{:130}

Depending on the parameters of the telegraph equation, the changes of the signal level distribution along the length of the single-dimensional transmission medium may take the shape of the simple wave, wave with decrement, or the diffusion-like pattern of the telegraph equation. The shape of the diffusion-like pattern is caused by the effect of the shunt capacitance.

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The solutions of the telegrapher's equations can be inserted directly into a circuit as components. The circuit in the top figure implements the solutions of the telegrapher's equations.^{ [14] }

The bottom circuit is derived from the top circuit by source transformations.^{ [15] } It also implements the solutions of the telegrapher's equations.

The solution of the telegrapher's equations can be expressed as an ABCD type * two-port network * with the following defining equations^{ [16] }

The ABCD type two-port gives and as functions of and . Both of the circuits above, when solved for and as functions of and yield exactly the same equations.

In the bottom circuit, all voltages except the port voltages are with respect to ground and the differential amplifiers have unshown connections to ground. An example of a transmission line modeled by this circuit would be a balanced transmission line such as a telephone line. The impedances Z(s), the voltage dependent current sources (VDCSs) and the difference amplifiers (the triangle with the number "1") account for the interaction of the transmission line with the external circuit. The T(s) blocks account for delay, attenuation, dispersion and whatever happens to the signal in transit. One of the T(s) blocks carries the *forward wave* and the other carries the *backward wave*. The circuit, as depicted, is fully symmetric, although it is not drawn that way. The circuit depicted is equivalent to a transmission line connected from to in the sense that , , and would be same whether this circuit or an actual transmission line was connected between and . There is no implication that there are actually amplifiers inside the transmission line.

Every two-wire or balanced transmission line has an implicit (or in some cases explicit) third wire which may be called shield, sheath, common, Earth or ground. So every two-wire balanced transmission line has two modes which are nominally called the differential and common modes. The circuit shown on the bottom only models the differential mode.

In the top circuit, the voltage doublers, the difference amplifiers and impedances Z(s) account for the interaction of the transmission line with the external circuit. This circuit, as depicted, is also fully symmetric, and also not drawn that way. This circuit is a useful equivalent for an unbalanced transmission line like a coaxial cable or a microstrip line.

These are not the only possible equivalent circuits.

- ↑ Reeve 1995 , p. 558
- 1 2 Chen 2004 , p. 26
- ↑ Terman 1943 , p. 112
- ↑ Kraus 1989 , pp. 380–419
- ↑ Hayt 1989 , pp. 382–392
- ↑ Marshall 1987 , pp. 359–378
- ↑ Sadiku 1989 , pp. 497–505
- ↑ Harrington 1961 , pp. 61–65
- ↑ Karakash 1950 , pp. 5–14
- ↑ Metzger 1969 , pp. 1–10
- ↑ Sadiku 1989 , pp. 501–503
- ↑ Marshall 1987 , pp. 369–372
- ↑ Miano, Giovanni; Maffucci, Antonio (2001).
*Transmission Lines and Lumped Circuits*. Academic Press. ISBN 0-12-189710-9. This book uses μ instead of α. - ↑ McCammon 2010
- ↑ Hayt 1971 , pp. 73–77
- ↑ Karakash 1950 , p. 44

In classical mechanics, a **harmonic oscillator** is a system that, when displaced from its equilibrium position, experiences a restoring force *F* proportional to the displacement *x*:

The **wave equation** is an important second-order linear partial differential equation for the description of waves—as they occur in classical physics—such as mechanical waves or light waves. It arises in fields like acoustics, electromagnetics, and fluid dynamics.

In physics and electrical engineering, a **cutoff frequency**, **corner frequency**, or **break frequency** is a boundary in a system's frequency response at which energy flowing through the system begins to be reduced rather than passing through.

In radio-frequency engineering, a **transmission line** is a specialized cable or other structure designed to conduct alternating current of radio frequency, that is, currents with a frequency high enough that their wave nature must be taken into account. Transmission lines are used for purposes such as connecting radio transmitters and receivers with their antennas, distributing cable television signals, trunklines routing calls between telephone switching centres, computer network connections and high speed computer data buses.

**Electrical impedance** is the measure of the opposition that a circuit presents to a current when a voltage is applied. The term *complex impedance* may be used interchangeably.

A **resistor–capacitor circuit**, or **RC filter** or **RC network**, is an electric circuit composed of resistors and capacitors driven by a voltage or current source. A first order RC circuit is composed of one resistor and one capacitor and is the simplest type of RC circuit.

The **Smith chart**, invented by Phillip H. Smith (1905–1987), is a graphical aid or nomogram designed for electrical and electronics engineers specializing in radio frequency (RF) engineering to assist in solving problems with transmission lines and matching circuits. The Smith chart can be used to simultaneously display multiple parameters including impedances, admittances, reflection coefficients, scattering parameters, noise figure circles, constant gain contours and regions for unconditional stability, including mechanical vibrations analysis. The Smith chart is most frequently used at or within the unity radius region. However, the remainder is still mathematically relevant, being used, for example, in oscillator design and stability analysis.

**Acoustic impedance** and **specific acoustic impedance** are measures of the opposition that a system presents to the acoustic flow resulting from an acoustic pressure applied to the system. The SI unit of acoustic impedance is the pascal second per cubic metre or the rayl per square metre, while that of specific acoustic impedance is the pascal second per metre or the rayl. In this article the symbol rayl denotes the MKS rayl. There is a close analogy with electrical impedance, which measures the opposition that a system presents to the electrical flow resulting from an electrical voltage applied to the system.

An **LC circuit**, also called a **resonant circuit**, **tank circuit**, or **tuned circuit**, is an electric circuit consisting of an inductor, represented by the letter L, and a capacitor, represented by the letter C, connected together. The circuit can act as an electrical resonator, an electrical analogue of a tuning fork, storing energy oscillating at the circuit's resonant frequency.

A network, in the context of electronics, is a collection of interconnected components. **Network analysis** is the process of finding the voltages across, and the currents through, every component in the network. There are many different techniques for calculating these values. However, for the most part, the applied technique assumes that the components of the network are all linear. The methods described in this article are only applicable to *linear* network analysis, except where explicitly stated.

In mathematics, the **Hamilton–Jacobi equation** (**HJE**) is a necessary condition describing extremal geometry in generalizations of problems from the calculus of variations, and is a special case of the Hamilton–Jacobi–Bellman equation. It is named for William Rowan Hamilton and Carl Gustav Jacob Jacobi.

The **Heaviside condition**, named for Oliver Heaviside (1850–1925), is the condition an electrical transmission line must meet in order for there to be no distortion of a transmitted signal. Also known as the **distortionless condition**, it can be used to improve the performance of a transmission line by adding loading to the cable.

**Ripple** in electronics is the residual periodic variation of the DC voltage within a power supply which has been derived from an alternating current (AC) source. This ripple is due to incomplete suppression of the alternating waveform after rectification. Ripple voltage originates as the output of a rectifier or from generation and commutation of DC power.

The **transmission coefficient** is used in physics and electrical engineering when wave propagation in a medium containing discontinuities is considered. A transmission coefficient describes the amplitude, intensity, or total power of a transmitted wave relative to an incident wave.

In electronics, a **differentiator** is a circuit that is designed such that the output of the circuit is approximately directly proportional to the rate of change of the input. An active differentiator includes some form of amplifier. A **passive differentiator circuit** is made of only resistors and capacitors.

A signal travelling along an electrical transmission line will be partly, or wholly, reflected back in the opposite direction when the travelling signal encounters a discontinuity in the characteristic impedance of the line, or if the far end of the line is not terminated in its characteristic impedance. This can happen, for instance, if two lengths of dissimilar transmission lines are joined together.

An **RLC circuit** is an electrical circuit consisting of a resistor (R), an inductor (L), and a capacitor (C), connected in series or in parallel. The name of the circuit is derived from the letters that are used to denote the constituent components of this circuit, where the sequence of the components may vary from RLC.

- Chen, Walter Y. (2004),
*Home Networking Basics*, Prentice Hall, ISBN 0-13-016511-5 - Harrington, Roger F. (1961),
*Time-Harmonic Electromagnetic Fields*, McGraw-Hill - Hayt, William H. (1971),
*Engineering Circuit Analysis*(second ed.), New York, NY: McGraw-Hill, ISBN 0070273820 - Hayt, William (1989),
*Engineering Electromagnetics*(5th ed.), McGraw-Hill, ISBN 0-07-027406-1 - Karakash, John J. (1950),
*Transmission Lines and Filter Networks*(1st ed.), Macmillan - Kraus, John D. (1984),
*Electromagnetics*(3rd ed.), McGraw-Hill, ISBN 0-07-035423-5 - Marshall, Stanley V. (1987),
*Electromagnetic Concepts & Applications*(1st ed.), Prentice-Hall, ISBN 0-13-249004-8 - Metzger, Georges; Vabre, Jean-Paul (1969),
*Transmission Lines with Pulse Excitation*, Academic Press - McCammon, Roy (June 2010),
*SPICE Simulation of Transmission Lines by the Telegrapher's Method*(PDF), retrieved 22 Oct 2010; also SPICE Simulation of Transmission Lines by the Telegrapher's Method (Part 1 of 3) - Reeve, Whitman D. (1995),
*Subscriber Loop Signaling and Transmission Handbook*, IEEE Press, ISBN 0-7803-0440-3 - Sadiku, Matthew N. O. (1989),
*Elements of Electromagnetics*(1st ed.), Saunders College Publishing, ISBN 0030134846 - Terman, Frederick Emmons (1943),
*Radio Engineers' Handbook*(1st ed.), McGraw-Hill

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