LC circuit

From Wikipedia, the free encyclopedia
Jump to: navigation, search
Linear analog electronic filters
edit
LC circuit diagram

An inductor-capacitor circuit (LC circuit) is an electric circuit composed of inductors and capacitors driven by a voltage or current source. A second order LC circuit is composed of one inductor and one capacitor and is the simplest type of LC circuit.

A second order LC circuit, also called a resonant circuit, tank circuit, or tuned circuit, consists of an inductor, represented by the letter L, and a capacitor, represented by the letter C. The circuit can act as an electrical resonator, an electrical analogue of a tuning fork, storing energy oscillating at the circuit's resonant frequency.

LC circuits are used either for generating signals at a particular frequency, or picking out a signal at a particular frequency from a more complex signal. They are key components in many electronic devices, particularly radio equipment, used in circuits such as oscillators, filters, tuners and frequency mixers.

An LC circuit is an idealized model since it assumes there is no dissipation of energy due to resistance. Any practical implementation of an LC circuit will always include loss resulting from small but non-zero resistance within the components and connecting wires. The purpose of an LC circuit is usually to oscillate with minimal damping, so the resistance is made as low as possible. While no practical circuit is without losses, it is nonetheless instructive to study this ideal form of the circuit to gain understanding and physical intuition. For a circuit model incorporating resistance, see RLC circuit.

Operation[edit]

Animated diagram showing the operation of a tuned circuit (LC circuit). The capacitor stores energy in its electric field E and the inductor stores energy in its magnetic field B (green). This jerky animation shows "snapshots" of the circuit at progressive points in the oscillation. The oscillations are slowed down; in an actual tuned circuit the charge oscillates back and forth tens of thousands to billions of times per second.

An LC circuit can store electrical energy oscillating at its resonant frequency. See the animation at right. A capacitor stores energy in the electric field (E) between its plates, depending on the voltage across it, and an inductor stores energy in its magnetic field (B), depending on the current through it.

If a charged capacitor is connected across an inductor, charge will start to flow through the inductor, building up a magnetic field around it and reducing the voltage on the capacitor. Eventually all the charge on the capacitor will be gone and the voltage across it will reach zero. However, the current will continue, because inductors resist changes in current. The energy to keep it flowing is extracted from the magnetic field, which will begin to decline. The current will begin to charge the capacitor with a voltage of opposite polarity to its original charge. When the magnetic field is completely dissipated the current will stop and the charge will again be stored in the capacitor, with the opposite polarity as before. Then the cycle will begin again, with the current flowing in the opposite direction through the inductor.

The charge flows back and forth between the plates of the capacitor, through the inductor. The energy oscillates back and forth between the capacitor and the inductor until (if not replenished by power from an external circuit) internal resistance makes the oscillations die out. Its action, known mathematically as a harmonic oscillator, is similar to a pendulum swinging back and forth, or water sloshing back and forth in a tank. For this reason the circuit is also called a tank circuit. The oscillation frequency is determined by the capacitance and inductance values. In typical tuned circuits in electronic equipment the oscillations are very fast, thousands to billions of times per second.

Resonance effect[edit]

The resonance effect occurs when inductive and capacitive reactances are equal in magnitude. The frequency at which this equality holds for the particular circuit is called the resonant frequency. The resonant frequency of the LC circuit is

\omega_0 =   {1 \over \sqrt{LC}}

where L is the inductance in henries, and C is the capacitance in farads. The angular frequency \omega_0\, has units of radians per second.

The equivalent frequency in units of hertz is

f_0 = { \omega_0 \over 2 \pi } = {1 \over {2 \pi \sqrt{LC}}}.

LC circuits are often used as filters; the L/C ratio is one of the factors that determines their "Q" and so selectivity. For a series resonant circuit with a given resistance, the higher the inductance and the lower the capacitance, the narrower the filter bandwidth. For a parallel resonant circuit the opposite applies. Positive feedback around the tuned circuit ("regeneration") can also increase selectivity (see Q multiplier and Regenerative circuit).

Stagger tuning can provide an acceptably wide audio bandwidth, yet good selectivity.

Applications[edit]

The resonance effect of the LC circuit has many important applications in signal processing and communications systems.

  1. The most common application of tank circuits is tuning radio transmitters and receivers. For example, when we tune a radio to a particular station, the LC circuits are set at resonance for that particular carrier frequency.
  2. A series resonant circuit provides voltage magnification.
  3. A parallel resonant circuit provides current magnification.
  4. A parallel resonant circuit can be used as load impedance in output circuits of RF amplifiers. Due to high impedance, the gain of amplifier is maximum at resonant frequency.
  5. Both parallel and series resonant circuits are used in induction heating.

LC circuits behave as electronic resonators, which are a key component in many applications:

Time domain solution[edit]

Kirchhoff's laws[edit]

By Kirchhoff's voltage law, the voltage across the capacitor, VC, plus the voltage across the inductor, VL must equal zero:

V _{C} + V_{L} = 0.\,

Likewise, by Kirchhoff's current law, the current through the capacitor equals the current through the inductor:

i_{C} = i_{L} .\,

From the constitutive relations for the circuit elements, we also know that

V _{L}(t) = L \frac{di_{L}}{dt}\,

and

i_{C}(t) = C \frac{dV_{C}}{dt}.\,

Differential equation[edit]

Rearranging and substituting gives the second order differential equation

\frac{d ^{2}i(t)}{dt^{2}} + \frac{1}{LC} i(t) = 0.\,

The parameter ω0, the resonant angular frequency, is defined as:

\omega_0 = { 1 \over \sqrt{LC} }

Using this can simplify the differential equation

\frac{d ^{2}i(t)}{dt^{2}} + \omega_0^ {2} i(t) = 0.\,

The associated polynomial is

  s^2 + \omega_0^2 = 0

Thus,

s = +j \omega_0\,

or

s = -j \omega_0\,
where j is the imaginary unit.

Solution[edit]

Thus, the complete solution to the differential equation is

i(t) = Ae ^{+j \omega_0 t}  +   Be ^{-j \omega_0  t}\,

and can be solved for A and B by considering the initial conditions.

Since the exponential is complex, the solution represents a sinusoidal alternating current.

Since the electric current i is a physical quantity, it must be real-valued. As a result, it can be shown that the constants A and B must be complex conjugates:

 A = B^*

Now, let

 A = {  I_0  \over 2  }  e^{j \phi }

Therefore,

 B = {  I_0  \over 2  }  e^{ -j \phi }

Next, we can use Euler's formula to obtain a real sinusoid with amplitude I 0, angular frequency ω0  = (LC)−1/2, and phase angle  \phi  .

Thus, the resulting solution becomes:

i(t) = I_0  \cos(\omega_0  t   +   \phi  ).\,

and

V (t) = L \frac{di}{dt}    = -\omega_0 L  I_0  \sin(\omega_0  t   +   \phi  )   \,

Initial conditions[edit]

The initial conditions that would satisfy this result are:

i(t=0) =   I_0  \cos(  \phi  ).\,

and

 V(t=0)   =    L \frac{di}{dt}(t=0) =  -\omega_0 L I_0  \sin( \phi   )       .\,

Series LC circuit[edit]

Series LC Circuit

In the series configuration of the LC circuit, the inductor L and capacitor C are connected in series, as shown here. The total voltage v across the open terminals is simply the sum of the voltage across the inductor and the voltage across the capacitor. The current i flowing into the positive terminal of the circuit is equal to the current flowing through both the capacitor and the inductor.

   v =  v_L   +   v_C   \,
    i  =  i_L   =   i_C  \,

Resonance[edit]

Inductive reactance magnitude (\scriptstyle X_L\,) increases as frequency increases while capacitive reactance magnitude (\scriptstyle X_C\,) decreases with the increase in frequency. At one particular frequency these two reactances are equal in magnitude but opposite in sign. The frequency at which this happens is called the resonant frequency (\scriptstyle f_0\,) for the given circuit.

Hence, at resonance:

X_L = -X_C\,
{\omega {L}} = {{1} \over {\omega} {C}}\,

Solving for  \scriptstyle \omega, we have

\omega = \omega_0 = { 1 \over \sqrt{LC}}

which is defined as the resonant angular frequency of the circuit.

Converting angular frequency (in radians per second) into frequency (in hertz), we have

f_0 =  {  \omega_0 \over  2 \pi}  = {1 \over {2 \pi \sqrt{LC}}}

In a series configuration, XC and XL cancel each other out. In real, rather than idealised components the current is opposed, mostly by the resistance of the coil windings. Thus, the current supplied to a series resonant circuit is a maximum at resonance.

  • In the limit as  \scriptstyle f  \to  f_0 current is maximum. Circuit impedance is minimum. In this state a circuit is called an acceptor circuit[citation needed].
  • For  \scriptstyle f < f_0 , \scriptstyle X_L \;\ll\; (-X_C)\,. Hence circuit is capacitive.
  • For  \scriptstyle f > f_0 , \scriptstyle X_L \;\gg\; (-X_C)\,. Hence circuit is inductive.

Impedance[edit]

In the series configuration, resonance occurs when the complex electrical impedance of the circuit approaches zero.

First consider the impedance of the series LC circuit. The total impedance is given by the sum of the inductive and capacitive impedances:

Z = Z_{L} + Z_{C}

By writing the inductive impedance as ZL = jωL and capacitive impedance as ZC = (jωC)−1 and substituting we have

Z(\omega) = j \omega L + \frac{1}{j{\omega C}} .

Writing this expression under a common denominator gives

Z(\omega) =  j \frac{(\omega^{2} L C - 1)}{\omega C} .

Finally, defining the natural angular frequency as

  \omega_0  =   {  1 \over  \sqrt{LC}   }

the impedance becomes

   Z(\omega) =  jL \bigg(  {  \omega^2 -  \omega_0^2  \over  \omega  }   \bigg) .

The numerator implies that in the limit as   \omega  \to  \pm  \omega_0   the total impedance Z will be zero and otherwise non-zero. Therefore the series LC circuit, when connected in series with a load, will act as a band-pass filter having zero impedance at the resonant frequency of the LC circuit.

Parallel LC circuit[edit]

Parallel LC Circuit

In the parallel configuration, the inductor L and capacitor C are connected in parallel, as shown here. The voltage v across the open terminals is equal to both the voltage across the inductor and the voltage across the capacitor. The total current i flowing into the positive terminal of the circuit is equal to the sum of the current flowing through the inductor and the current flowing through the capacitor.

   v =  v_L   =    v_C   \,
    i  =  i_L   +    i_C  \,

Resonance[edit]

Let R be the internal resistance of the coil. When XL equals XC, the reactive branch currents are equal and opposite. Hence they cancel out each other to give minimum current in the main line. Since total current is minimum, in this state the total impedance is maximum.

Resonant frequency given by: f_0 =  { \omega_0  \over 2 \pi }   = {1 \over {2 \pi \sqrt{LC}}} .

Note that any reactive branch current is not minimum at resonance, but each is given separately by dividing source voltage (V) by reactance (Z). Hence I=V/Z, as per Ohm's law.

  • At f0, line current is minimum. Total impedance is maximum. In this state a circuit is called a rejector circuit[citation needed].
  • Below f0, circuit is inductive.
  • Above f0,circuit is capacitive.

Impedance[edit]

The same analysis may be applied to the parallel LC circuit. The total impedance is then given by:

Z = \frac{Z_{L}Z_{C}}{Z_{L} + Z_{C}}

and after substitution of \scriptstyle Z_{L} and \scriptstyle Z_{C} and simplification, gives

   Z(\omega) =   -j  \frac{ \omega L}{\omega^{2}LC-1}

which further simplifies to

   Z(\omega)   =   -j \bigg({1 \over C } \bigg)   \bigg( \frac{ \omega }{\omega^{2}  - \omega_0^2  }   \bigg)

where

  \omega_0 = {   1   \over   \sqrt{LC}}

Note that

 \lim_{\omega   \to \pm   \omega_0 }   Z(\omega) = \infty

but for all other values of \scriptstyle \omega  the impedance is finite. The parallel LC circuit connected in series with a load will act as band-stop filter having infinite impedance at the resonant frequency of the LC circuit. The parallel LC circuit connected in parallel with a load will act as band-pass filter.

History[edit]

The first evidence that a capacitor and inductor could produce electrical oscillations was discovered in 1826 by French scientist Felix Savary.[1][2] He found that when a Leyden jar was discharged through a wire wound around an iron needle, sometimes the needle was left magnetized in one direction and sometimes in the opposite direction. He correctly deduced that this was caused by a damped oscillating discharge current in the wire, which reversed the magnetization of the needle back and forth until it was too small to have an effect, leaving the needle magnetized in a random direction. American physicist Joseph Henry repeated Savary's experiment in 1842 and came to the same conclusion, apparently independently.[3][4] British scientist William Thomson (Lord Kelvin) in 1853 showed mathematically that the discharge of a Leyden jar through an inductance should be oscillatory, and derived its resonant frequency.[1][3][4] British radio researcher Oliver Lodge, by discharging a large battery of Leyden jars through a long wire, created a tuned circuit with its resonant frequency in the audio range, which produced a musical tone from the spark when it was discharged.[3] In 1857, German physicist Berend Wilhelm Feddersen photographed the spark produced by a resonant Leyden jar circuit in a rotating mirror, providing visible evidence of the oscillations.[1][3][4] In 1868, Scottish physicist James Clerk Maxwell calculated the effect of applying an alternating current to a circuit with inductance and capacitance, showing that the response is maximum at the resonant frequency.[1] The first example of an electrical resonance curve was published in 1887 by German physicist Heinrich Hertz in his pioneering paper on the discovery of radio waves, showing the length of spark obtainable from his spark-gap LC resonator detectors as a function of frequency.[1]

One of the first demonstrations of resonance between tuned circuits was Lodge's "syntonic jars" experiment around 1889.[1][3] He placed two resonant circuits next to each other, each consisting of a Leyden jar connected to an adjustable one-turn coil with a spark gap. When a high voltage from an induction coil was applied to one tuned circuit, creating sparks and thus oscillating currents, sparks were excited in the other tuned circuit only when the circuits were adjusted to resonance. Lodge and some English scientists preferred the term "syntony" for this effect, but the term "resonance" eventually stuck.[1] The first practical use for LC circuits was in the 1890s in spark-gap radio transmitters to allow the receiver and transmitter to be tuned to the same frequency. The first patent for a radio system that allowed tuning was filed by Lodge in 1897, although the first practical systems were invented in 1900 by Italian radio pioneer Guglielmo Marconi.[1]

See also[edit]

References[edit]

  1. ^ a b c d e f g h Blanchard, Julian (October 1941). "The History of Electrical Resonance". Bell System Technical Journal (USA: American Telephone & Telegraph Co.) 20 (4): 415–. doi:10.1002/j.1538-7305.1941.tb03608.x. Retrieved 2011-03-29. 
  2. ^ Savary, Felix (1827). "Memoirs sur l'Aimentation". Annales de Chimie et de Physique (Paris: Masson) 34: 5–37. 
  3. ^ a b c d e Kimball, Arthur Lalanne (1917). A College Text-book of Physics, 2nd Ed.. New York: Henry Hold and Co. pp. 516–517. 
  4. ^ a b c Huurdeman, Anton A. (2003). The worldwide history of telecommunications. USA: Wiley-IEEE. pp. 199–200. ISBN 0-471-20505-2. 

External links[edit]