Home / Technical Articles / Lecture Notes In DC Electric Sources and Principles Of Electrical Circuits

Introduction to DC sources

DC sources refer to sources of electrical energy which are associated with constant voltages and currents. A DC power supply can be constructed as an electronic circuit operating from the ac mains electricity supply and designed for purpose.

Lecture Notes In DC Electric Sources and Principles Of Electrical Circuits
Lecture Notes In DC Electric Sources and Principles Of Electrical Circuits

Alternatively it can be obtained from a battery, with the latter being used in portable equipment and machines where a connection to the mains ac supply is not convenient or practical.

DC circuits essentially contain only DC power sources and resistive elements and therefore form a suitable basis for studying the fundamental principles of electrical circuit analysis.

Let’s break this article into few sections and start the lecture notes:

    1. Few Words About Batteries
      1. Disposable Battery
      2. Rechargeable Battery
      3. Battery Construction
    2. The Ideal Voltage Source
    3. The Ideal Current Source
    4. The Non-Ideal Voltage Source
    5. The Non-Ideal Current Source
    6. Energy Expenditure and Power Dissipation

1. Few Words About Batteries

The DC battery is common place today. Batteries are used in the widest range of scenarios, from the smallest applications in hearing aids and small digital watches to the large heavy-duty lead acid batteries used in the automotive industry.

The voltage cell was invented by Alessandro Volta (1745-1827), an Italian physicist in 1792 during his work on electrolysis and the first battery as a stack of such cells in 1800.

Voltaic pile, an early form of battery by Alessandro Volta in Italy, based on previous works by Luigi Galvani
Figure 0 – Voltaic pile, an early form of battery by Alessandro Volta in Italy, based on previous works by Luigi Galvani

Today, the term cell and battery are used almost interchangeably, but many low-voltage batteries are in fact single voltaic cells while strictly-speaking a battery is a number of cells stacked in series to obtain higher voltages than a single cell can provide.

A battery is essentially a source of DC electrical energy. It converts stored chemical energy into electrical energy through an electrochemical process. This then provides a source of electromotive force or emf to enable currents to flow in electric and electronic circuits.

There are basically two classes of battery, disposable and rechargeable.

1.1. Disposable Battery

The disposable battery, as the name suggests, is intended for a single use only, so that once the energy contained within the chemical constituents of battery is converted into electrical form then the battery is ‘used up’ and is disposed of.

These batteries are sometimes referred to as primary cells and include the common Zinc-Carbon (ZnC) AAA, AA, C and D cells or their equivalent alkaline Manganese-Dioxide (MnO2) versions as well as the myriad of small button cells using Zinc-Oxide (ZnO), Silver-Oxide (AgO) or ChromiumDioxide (CrO2) among other materials.

Go back to contents ↑

1.2. Rechargeable Battery

The second class of battery is the well known rechargeable type, which has gained widely increased usage in the past two or three decades.

In this type of battery when the chemical energy stored has been used up it can be replaced by a reversal of the chemical process through the use of electricity to ‘recharge’ it which can be done from a mains supply.

Thus the charge stored by this type of battery can be replenished and the battery can be used in sequential charge and recharge cycles.

Eventually however, the materials in a rechargeable battery degrade and it reaches the end of its life. Rechargeable batteries include the equivalent of the standard cells such as Nickel-Cadmium (NiCd) or Nickel-Metal Hydride (NiMH) or the higher voltage Lithium-Ion (Li-ion) cells right up to the classic Lead-Acid (PbH2SO4) car battery.

Go back to contents ↑

1.3. Battery Construction

The construction and use of a typical C or D type cell is illustrated in Figure 1. The outer metal case in the form of a cylindrical container is made of Zinc and acts as the negative electrode of the cell. Its base also serves as the negative terminal of the battery.

The cylinder is filled with a chemical compound which acts as an electrolyte.

In modern batteries this is in non-liquid form of a paste or dry compound.

The positive electrode of the cell takes the form of a Carbon or Graphite rod with a metal cap which is inserted into the electrolyte in the centre of the cylinder. The metal cap on the rod serves as the positive terminal of the battery.

The Construction and Operation of a Battery
Figure 1 – The Construction and Operation of a Battery

When a conducting resistive load is connected between the positive and negative terminals of the battery a closed electrical circuit is formed. Under this condition a number of chemical reactions take place in the electrolyte which results in the generation of positively charged ions and free negatively charged electrons within it.

The positive ions migrate through the electrolyte towards the carbon rod and become deposited on it. The electrons, on the other hand, cannot migrate through the electrolyte because its chemical composition forms a barrier which inhibits the passage of electrons through it.

Instead, the electrons accumulate at the negative electrode of the cell. This gives rise to a potential difference between the two terminals of the battery, which results in an emf or electric field across the resistive load connected between them. The emf then causes the electrons to flow in the external electric circuit through the load and finally to the positive terminal of the battery.

This gives rise to a continuous flow of current in the electric circuit.

In the circuit shown in Figure 1 the electrical load is the light bulb and the energy drawn from the battery by the bulb is emitted as visible light. As long as the closed electric circuit exists the current continues to flow and the electrochemical process in the electrolyte continues with the constituent chemicals being converted into other chemicals.

Eventually the supply of original chemicals in the electrolyte becomes depleted and the emf generated between the terminals of the battery drops, ultimately to zero, and the battery becomes discharged.

At this stage a disposable battery is discarded, while a rechargeable battery will be placed on a charger which reverses the electrochemical process in the electrolyte and restores charge to the battery by passing an electric current through it in the reverse direction for a sufficient period of time.

Thus it can be seen that there is a limit to the length of time for which a battery can generate electricity and consequently has a limited lifetime or cycle time.

The length of time for which a battery lasts is determined by the amount of charge it stores in total and the rate at which this charge is used, which in turn depends on the magnitude of the current drawn from it.

A battery will last longer when a low value of current is drawn from it than it will when a high value of current is demanded.

This is indicated in Figure 2, where the terminal voltage of a battery is plotted against time for different values of current drawn from it with I4 > I3 > I2 > I1.

The Discharge Profile of a Battery at Different Currents
Figure 2 – The Discharge Profile of a Battery at Different Currents

The operating lifetime (disposable) or cycle time (rechargeable) depends essentially on the amount of charge it stores in the electrolyte, which can be converted into free electrons to provide the current in an electric circuit.

One might then expect this battery capacity to be expressed as a quantity of charge in Coulombs.

However, in practice, it proves more useful to express the battery capacity in terms of the product of current (in Amperes) and time (in hours). Battery capacity is therefore expressed in units of Ampere-hours (Ahr).

This allows the effective lifetime of the battery to be calculated for different levels of current drawn from it as indicated in Table 1.

Table 1 – Battery Lifetime vs Current Drawn

Battery CapacityCurrent DrawnLifetime
10 Ahr10 A1 hr
10 Ahr1 A10 hr
10 Ahr20 A30 mins
10 Ahr0.25 A40 hrs
1 Ahr1 A1 hr
1 Ahr5 A12 mins
1 Ahr100 mA10 hr

It is also important, however, to realise that in practice there is a maximum current which a battery is able to deliver and this must also be taken into account when choosing a suitable battery for a particular application.

For example, the 1 Ahr battery of Table 1 may not be able to deliver a current as high as 5A due to the limitations of its chemistry and in this case could not be used in a scenario where this level of current is demanded, even for the short period of 12 mins.

Go back to contents ↑

2. The Ideal Voltage Source

The symbol already used for a DC battery is used for an ideal DC voltage source as shown in Figure 3. The emf of an ideal battery is the sum of the cell voltages which are stacked to obtain a higher voltage than a single cell can provide.

The voltage measured between the terminals of the battery is the output voltage, VO. The load connected to the battery is shown as a single resistor, RL, which could of course represent the equivalent resistance of a more complicated resistive configuration. The current drawn from the voltage source and flowing through the load resistance is labelled, IL.

An ideal voltage source is one which provides a constant output voltage regardless of the load placed on it.

An Ideal Voltage Source Driving a Resistive Load
Figure 3 – An Ideal Voltage Source Driving a Resistive Load

The definitive characteristic of the ideal voltage source is therefore:

VO = E

That is, the output or terminal voltage of the battery as measured between its positive and negative terminals is always the internal collective cell voltage, E.

Since the output voltage of the battery, VO, is in this case identical to the voltage across the single load resistor VL, then from Ohm’s law we have:

IL = V/ RL = E / RL

This shows that the current through the load is a function of the resistance, RL, with the voltage across the load being independent of it.

This implies that the source is capable of providing whatever current is demanded of it. This in turn suggests that if a ‘short-circuit’ is placed across the source with R= 0 then the current would be unlimited with IL → ∞.

Clearly, a situation like this cannot prevail in reality.

For example, if a piece of heavy-duty conducting cable were placed across a 12V lead-acid car battery, the battery would rapidly overheat, vent Hydrogen gas, melt and possibly explode. Therefore, the concept of a short-circuit load is primarily a theoretical one to be used only on paper for the purposes of circuit analysis.

However, there are scenarios in practice where electronic equipment must be protected against damage in the event of a short-circuit occurring unintentionally or inadvertently.

Go back to contents ↑

3. The Ideal Current Source

It is sometimes necessary to generate a defined and constant value of current to drive a circuit or load rather than a constant voltage. This is known as a current source, the most common symbol for which used is the double overlapping circles shown in Figure 4.

Note that the direction of the current generated to flow out of the terminals of the source must be indicated in some manner, usually by a directed arrow.

Current sources do not occur naturally in cell form like batteries and are constructed using electronic circuits which are in turn powered from a voltage source.

An Ideal Current Source Driving a Resistive Load
Figure 4 – An Ideal Current Source Driving a Resistive Load

The definitive characteristic of the ideal current source is that:

IL = I

That is, the current which flows out of the positive terminal of the current source, around the circuit through the load resistor, RL, and back into the negative terminal of the source is always equal to the nominal value of the current source, I.

This value is independent of the value of the load resistance, RL. The voltage developed across the load, VL, is given by Ohm’s law as:


This shows that the voltage across the load, which is also the voltage which is developed across the current source itself, is a function of the resistance, RL.

A battery charger is a good working example of a current source. The current source is powered from mains electricity and the user sets the value of the constant current while the battery to be charged forms the load as illustrated by the set-up shown in Figure 5 below.

The voltage developed across the terminal of the current source will adjust itself to be equal to the battery voltage.

A Constant Current Source Used to Charge a Battery
Figure 5 – A Constant Current Source Used to Charge a Battery

Go back to contents ↑

4. The Non-Ideal Voltage Source

In practice a voltage source is not ideal and does not provide unlimited current. When the battery or voltage source is not connected to a load, the voltage between its terminals is referred to as its open-circuit terminal voltage, VOC, and is essentially the same as the cell voltage, E.

However, when a load is connected to the source, the terminal voltage drops as current is drawn from it so that:

VO < E or VO < VOC

This effect can be observed in the curves shown in Figure 2 where the voltage available from the battery is slightly lower than the open circuit voltage, VOC, and the drop in voltage becomes more pronounced as the current drawn from the battery is increased.

This effect can be modelled by attributing an internal or source resistance, RS, to the non-ideal voltage source.

This can then be represented as an ideal voltage source generating the cell voltage, E, with an internal source resistance, RS connected in series with the ideal source and its output terminals as shown in Figure 6.

In this case the current drawn from the supply flows through the internal source resistance, RS, giving rise to a potential drop across it, VS.

In this case by Kirchhoff’s Law:

VO = E − VS

But from Ohm’s Law:


An Non-Ideal Voltage Source Driving a Resistive Load
Figure 6 – An Non-Ideal Voltage Source Driving a Resistive Load

so that:


Note also that for the load:


From the relation for resistors connected in series we have:

IL = E / (RL + RS)

So that finally:

VL = RL E / (RL + RS)

This shows that there is essentially a potential divider action between the internal resistance of the voltage source, RS, and the resistance of the load, RL, with the same current flowing through both resistances.

This has the effect of reducing the effective output voltage of the battery.

Go back to contents ↑

5. The Non-Ideal Current Source

In a similar manner in practice, a current source is not ideal. The output current provided by a non-ideal current source varies slightly with a change in the load resistance connected to it. This effect can be modelled by attributing an internal resistance to the current source in a similar manner to the non-ideal voltage source.

However, the internal resistance is connected across the ideal current source in this case rather than in series with it as shown in Figure 7.

A Non-Ideal Current Source Driving a Resistive Load
Figure 7 – A Non-Ideal Current Source Driving a Resistive Load

In the case of the non-ideal current source the internal resistance, RS, is much higher than that in the case of the non-ideal voltage source.

The effect of the internal resistance in the non-ideal current source is to shunt some of the current generated by the ideal current source, I, so that the current which flows through the load, IL, is less than the ideal value.

In this case:

IL < I

The degree of drop in the output current from the ideal value depends on the value of the load resistance, RL, by comparison with the internal source resistance, RS.

If Kirchhoff’s Current Law is applied to the positive output terminal of the current source we have:

I = IS + IL

From previous work on current splitting between resistors in parallel:

IL = RSI / (RS + RL)

This shows that there is essentially a current splitting action between the internal source resistance, RS and the load resistance, RL.

Note also that for the load:


so that:

VL = RSRLI / (RS + RL)

Go back to contents ↑

6. Energy Expenditure and Power Dissipation

In the circuits above the load resistance, RL, represents the electrical equivalent of some form of load which demands or uses energy.

For example, when the bulb in a torch powered by batteries lights up, electrical energy is drawn from the batteries and converted into light. This uses up the energy stored in the batteries and the rate at which the energy is depleted depends on the brightness of the bulb, often referred as its wattage.

The question is simply what energy or power does the electrical load dissipate?

If it is recalled that power dissipated is the rate at which energy is expended per unit time, then:

Power formulae

The unit of Energy is the Joule (J), called after the English physicist James Prescott Joule (1818-89), who discovered the first law of thermodynamics. The unit of power is the Watt (W), named after James Watt (1736-1819), a Scottish mechanical engineer and developer of the steam engine.

Then for a resistive element in an electric circuit with a potential drop, V across it and a current, I flowing through it we have:

P = VI

But from Ohm’s Law we recall:

V = IR or I = V / R

so that:

P = VI = I2 R = V2 / R

Go back to contents ↑

Reference // DC Circuit Analysis – Lecture 5: DC Electric Sources, Energy and Power

SEARCH: Articles, software & guides

Premium Membership

Premium membership gives you an access to specialized technical articles and extra premium content (electrical guides and software).
Get Premium Now ⚡

About Author


Edvard Csanyi

Electrical engineer, programmer and founder of EEP. Highly specialized for design of LV/MV switchgears and LV high power busbar trunking (<6300A) in power substations, commercial buildings and industry fascilities. Professional in AutoCAD programming. Present on


  1. Murugesan
    May 26, 2018

    Excellent article

    May 18, 2018

    After long time, good article was published on DC Sources of BATTERYS by EDWARD.. Lot of thanks for your effort.

  3. Bendi abdellah
    May 17, 2018

    The work you are doing in the field of electrical engineering is very useful and rich of information for various categories of people interested in electrical theories and practices. I appreciate a lot the effor

    of all those making it possible benefit

  4. zaid nazik
    May 16, 2018

    I feel so appreciated with the articles news lectures ….etc you made
    i am following all articles hope more prosperious

Leave a Comment

Tell us what you're thinking... we care about your opinion!

Premium Membership

Get access to premium electrical guides, technical articles and much more!