### The LR Series Circuit

The above *LR series circuit* is connected across a constant voltage source, (the battery) and a switch. Assume that the switch, S is open until it is closed at a time t = 0, and then remains permanently closed producing a “step response” type voltage input. The current, i begins to flow through the circuit but does not rise rapidly to its maximum value of Imax as determined by the ratio of V / R (Ohms Law).

This limiting factor is due to the presence of the self induced emf within the inductor as a result of the growth of magnetic flux, (Lenz’s Law). After a time the voltage source neutralizes the effect of the self induced emf, the current flow becomes constant and the induced current and field are reduced to zero.

We can use Kirchhoff’s Voltage Law, (KVL) to define the individual voltage drops that exist around the circuit and then hopefully use it to give us an expression for the flow of current.

Kirchhoff’s voltage law (KVL) gives us:

The voltage drop across the resistor, R is I*R (Ohms Law).

The voltage drop across the inductor, L is by now our familiar expression L(di/dt)

Then the final expression for the individual voltage drops around the LR series circuit can be given as:

We can see that the voltage drop across the resistor depends upon the current, i, while the voltage drop across the inductor depends upon the rate of change of the current, di/dt. When the current is equal to zero, ( i = 0 ) at time t = 0 the above expression, which is also a first order differential equation, can be rewritten to give the value of the current at any instant of time as:

### Expression for the Current in an LR Series Circuit

- Where:
- V is in Volts
- R is in Ohms
- L is in Henries
- t is in Seconds
- e is the base of the Natural Logarithm = 2.71828

The **Time Constant**, ( τ ) of the LR series circuit is given as L/R and in which V/R represents the final steady state current value after five time constant values. Once the current reaches this maximum steady state value at 5τ, the inductance of the coil has reduced to zero acting more like a short circuit and effectively removing it from the circuit.

Therefore the current flowing through the coil is limited only by the resistive element in Ohms of the coils windings. A graphical representation of the current growth representing the voltage/time characteristics of the circuit can be presented as.

### Transient Curves for an LR Series Circuit

Since the voltage drop across the resistor, V_{R} is equal to I*R (Ohms Law), it will have the same exponential growth and shape as the current. However, the voltage drop across the inductor, V_{L} will have a value equal to: Ve^{(-Rt/L)}. Then the voltage across the inductor, V_{L} will have an initial value equal to the battery voltage at time t = 0 or when the switch is first closed and then decays exponentially to zero as represented in the above curves.

The time required for the current flowing in the LR series circuit to reach its maximum steady state value is equivalent to about **5 time constants** or 5τ. This time constant τ, is measured by τ = L/R, in seconds, where R is the value of the resistor in ohms and L is the value of the inductor in Henries. This then forms the basis of an RL charging circuit were 5τ can also be thought of as “5*(L/R)” or the *transient time* of the circuit.

The transient time of any inductive circuit is determined by the relationship between the inductance and the resistance. For example, for a fixed value resistance the larger the inductance the slower will be the transient time and therefore a longer time constant for the LR series circuit. Likewise, for a fixed value inductance the smaller the resistance value the longer the transient time.

However, for a fixed value inductance, by increasing the resistance value the transient time and therefore the time constant of the circuit becomes shorter. This is because as the resistance increases the circuit becomes more and more resistive as the value of the inductance becomes negligible compared to the resistance. If the value of the resistance is increased sufficiently large compared to the inductance the transient time would effectively be reduced to almost zero.

## LR Series Circuit Example No1

A coil which has an inductance of 40mH and a resistance of 2Ω is connected together to form a LR series circuit. If they are connected to a 20V DC supply.

**a).** What will be the final steady state value of the current.

**b)** What will be the time constant of the RL series circuit.

**c)** What will be the transient time of the RL series circuit.

**d)** What will be the value of the induced emf after 10ms.

**e)** What will be the value of the circuit current one time constant after the switch is closed.

The Time Constant, τ of the circuit was calculated in question b) as being 20ms. Then the circuit current at this time is given as:

You may have noticed that the answer for question (e) which gives a value of 6.32 Amps at one time constant, is equal to 63.2% of the final steady state current value of 10 Amps we calculated in question (a). This value of 63.2% or 0.632 x I_{MAX} also corresponds with the transient curves shown above.

## Power in an LR Series Circuit

Then from above, the instantaneous rate at which the voltage source delivers power to the circuit is given as:

The instantaneous rate at which power is dissipated by the resistor in the form of heat is given as:

The rate at which energy is stored in the inductor in the form of magnetic potential energy is given as:

Then we can find the total power in a RL series circuit by multiplying by i and is therefore:

Where the first I^{2}R term represents the power dissipated by the resistor in heat, and the second term represents the power absorbed by the inductor, its magnetic energy.

### AC Inductor Phasor Diagram

These voltage and current waveforms show that for a purely inductive circuit the current lags the voltage by 90^{o}. Likewise, we can also say that the voltage leads the current by 90^{o}. Either way the general expression is that the current lags as shown in the vector diagram. Here the current vector and the voltage vector are shown displaced by 90^{o}. *The current lags the voltage*.

We can also write this statement as, V_{L} = 0^{o} and I_{L} = -90^{o} with respect to the voltage, V_{L}. If the voltage waveform is classed as a sine wave then the current, I_{L} can be classed as a negative cosine and we can define the value of the current at any point in time as being:

Where: ω is in radians per second and t is in seconds.

Since the current always lags the voltage by 90^{o} in a purely inductive circuit, we can find the phase of the current by knowing the phase of the voltage or vice versa. So if we know the value of V_{L}, then I_{L} must lag by 90^{o}. Likewise, if we know the value of I_{L} then V_{L} must therefore lead by 90^{o}. Then this ratio of voltage to current in an inductive circuit will produce an equation that defines the **Inductive Reactance**, **X _{L}** of the coil.

### Inductive Reactance

We can rewrite the above equation for inductive reactance into a more familiar form that uses the ordinary frequency of the supply instead of the angular frequency in radians, ω and this is given as:

Where: ƒ is the Frequency and L is the Inductance of the Coil and 2πƒ = ω.

From the above equation for inductive reactance, it can be seen that if either of the **Frequency** or **Inductance** was increased the overall inductive reactance value would also increase. As the frequency approaches infinity the inductors reactance would also increase to infinity acting like an open circuit.

However, as the frequency approaches zero or DC, the inductors reactance would decrease to zero, acting like a short circuit. This means then that inductive reactance is “proportional” to frequency.

In other words, inductive reactance increases with frequency resulting in X_{L} being small at low frequencies and X_{L} being high at high frequencies and this demonstrated in the following graph:

### Inductive Reactance against Frequency

The slope shows that the “Inductive Reactance” of an inductor increases as the supply frequency across it increases.Therefore Inductive Reactance is proportional to frequency giving: ( X_{L} α ƒ ) |

Then we can see that at DC an inductor has zero reactance (short-circuit), at high frequencies an inductor has infinite reactance (open-circuit).