The Dreaded Ohms Law

In a previous article we looked at the power formula, and discussed the relationship between power, voltage and current. Having looked at the power formula, there is now only one more formula needed to help solve just about every electrical calculation, this is the dreaded Ohms law. We wont get involved with deriving the formula, but take a minute to read the following illustration:

garden_hoseWhen you turn the tap on connected to a garden hose without a nozzle, you will see water flowing out the other end. The flow of water through the hose  is similar to electric current flow – electric current is the flow of electrons through a wire.

If you now put your thumb on the end of the hose and try to block the water flow, the water pressure you feel is like voltage. Voltage is the pressure which pushes the electrons through the wire. What is interesting is that if your thumb completely blocks the water flow, there is still water pressure (voltage). Having a nozzle on the end of the hose and stopping the water flow is like having a wall power socket with nothing plugged in – there is no water/current flow, but the pressure/voltage is still there. The point to note is that voltage is present, even if there is no current flowing. Another example of this is a car battery – it always has 12 volts available to any wire connected to it, no matter what the current drawn.

Back to the garden hose, if you now move your thumb around on the end of the hose, you can vary the amount of water which comes out. That is, as you vary the resistance to the water, you vary the flow. This is same in an electrical circuit – vary the resistance and the current flow changes accordingly.  Let’s define electrical resistance as “that which resists, blocks, impedes or restricts current flowing through a circuit”. Examples of a resistance in a circuit are a light bulb or an electrical appliance.

If the voltage (water pressure) remains the same, the current flow will depend on the resistance. The greater the resistance, the less the current flow. Conversely, the less the resistance, the greater the current flow. This is like the more you block the end of the hose the more the water flow decreases, reducing the resistance increases the water flow.

Georg Simon Ohm
Georg Simon Ohm

If the resistance remains the same, the current flow can be increased or decreased by increasing or decreasing the voltage (water pressure).

In 1827, a German named Georg Simon Ohm published a book describing the relationship between voltage, current flow and resistance. This relationship is now known as Ohms Law.  Ohms law states that current flow is directly proportional to voltage, and inversely proportional to resistance.

Mathematically, it looks like this:

 Current = Voltage/Resistance

The symbols and units of measurement for voltage and current are the same as for the power formula. Note the standard terms for resistance.

 NameSymbolUnits of Measurement
CurrentIamperes or amps (A)
VoltageVvolts (V)
ResistanceRohms (Ω)

Therefore, we can write this formula quickly as:

 I = V/R

A popular way to remember this formula and its derivatives is by the triangle shown here. Whatever characteristic you are looking for, place your finger to cover that, and the formula you need remains.ohms law triangle volts current resistance

Example 1: To find the voltage of a circuit when you know the resistance and the current, place a finger to cover the “V”, and the formula is I x R.

Example 2: To find the current in a circuit when you know the voltage and resistance, place a finger to cover the “I”, and the formula is V/R

Example 3: To find the resistance of a circuit when you know the voltage and current, place a finger to cover the “R”, and the formula is V/I

In other words, the formula in its three possible forms is:

 V = I x R              I = V/R                  R = V/I

Using these formulas and the following circuit, the relationship between resistance and current can be seen, given that the voltage remains the same.

Example 1: Given that the voltage is 220 Volts, and the resistance is 110 ohms(Ω), we can ohms law triangle volts current resistancecalculate the current using the formula:

I = V/R = 220/110 = 2 Amps

Example 2: Same voltage (220 Volts), but now the resistance is only 2Ω.

I = V/R = 220/2 = 110 Amps

That is, the greater the resistance, the less the current allowed to flow. Also the less the resistance, the greater the current allowed to flow.

Using the water analogy again may be useful. If you had a large diameter water pipe, then a lot of water (current) could flow through it because the “resistance” is low (no blockages). If there is a blockage in the pipe (resistance), then the (current) flow is reduced. The greater the blockage (the higher resistance), the less the (current) flow.

This principle is illustrated in the examples above. In example 1, a resistance of 110Ω allowed only 2 amps to flow through the circuit. In example 2, a small resistance (2Ω) allowed a large current of 110 amps to flow through the circuit.

Resistance is anything that resists current flowing through a circuit. A light bulb is a resistance, as is an iron, a food processor, or a stove. In electronics, there are little components called resistors, which are made to be a fixed known value. Even just plain cable has some resistance, in fact, the reason to have thick cables is to reduce the resistance and allow more current to flow through it (like a fire hose is larger than a garden hose  – so more water can flow through it).

P.S.: we have just covered the basic principles of Ohms Law, but shhh, don’t tell anyone.

If you find the maths confusing, try the simple Ohm’s law calculator.

Series or Parallel

Often you don’t know what the resistance in a circuit is, nor do you need to know. However these formulas are still very useful, but mainly for what is derived from them, rather than for their immediate calculation. This is a long-winded way of saying, “please accept that the following concepts are derived from the above formula, without us having to waste time and effort proving it”.

Concept 1:

Consider this circuit of six light bulbs. Because they are connected one after the other, they are said to be connected in series.

series circuit volts currentWhat is interesting is what happens with the voltage, current and resistance.

Voltage: The “voltage in” is the sum of the voltages across all the individual lights. In this example, the individual voltage across each light is 40 volts, so the total voltage is 240 volts.

Current: The current through each individual light is the same as the current throughout the whole circuit. If the current going to the circuit is 1 amp, then the current through each individual light is also 1 amp.

Resistance: The total resistance equals the sum of all the individual “series” resistances.

In practice this type of circuit isn’t used much in a house. This is because if 240 volts comes into the house, and there are six lights in series, then each light would only be getting one English: Closeup of a string of decorative Chr...sixth of that voltage i.e. 40 volts. However, this type of circuit is often used for Christmas tree lights e.g. 20 lights at 12 Volts each equals 240 Volts. The problem with this circuit is that if one light blows, then all the others go out also. This is because the wire connection to the next light is broken, so the circuit is not complete.

A series circuit is often used with batteries. When batteries are in series, the total voltage equals the sum of all the individual voltages, and the total current flowing through the whole circuit is the same as the current flowing through any one battery. For example: four 1.5 volt 500mA batteries in series with each other makes a battery of 6 volts (4 x 1.5) @500mA.


Consider this circuit of six light bulbs. Because they are connected across each other, or in parallel with each other, they are said to be connected in parallel.

parallel circuit volts current

What happens with the voltage, current and resistance in this type of circuit is in contrast with what happens in a series circuit.

Voltage: The voltage across each light is the same as the “voltage in”. If 220 volts is coming in to the circuit, then there is 220 volts across each individual light.

Current: The current going into the circuit is the sum of the currents in each individual light. If the current through each light is 1 amp, then the total current coming into this circuit would be 6 amps (6 x 1 amp).

Resistance: The total resistance is calculated by a complicated formula that we don’t need to learn at this stage. Suffice to say that the total resistance is less than the lowest individual resistance. Here is the formula for those who really need to know:

parallel resistanceIn practice this type of circuit is used in houses. e.g. If you have 220 volts coming into your house, then all the lights and power outlets (power sockets) are also 220 volts because they are connected in parallel.

Batteries can also be connected in parallel. The output voltage of two batteries in parallel is the same as one of the batteries, but the current capacity is doubled. For Example: two 12 volt 100 amp/hour car batteries in parallel make up the equivalent of a 12 volt 200 amp/hour battery. The same two batteries in series would make the equivalent of a 24 volt 100 amp/hour battery.

Putting it all Together

Some people are excited by the way that the Ohm’s law formula can be substituted into our Power formula to create new formulas. For those of you who like to play with formulas, you can work out how this is done; for the rest, just accept that this table shows the various combinations of these formulas.

power chart volts currrent resistance
This table displays all the possible combinations using the two basic formulas we have learned. Try using a calculator and the following values to check it out:

V = 12 volts          I = 2 amps           R = 6Ω           P = 24 watts

You might like to print the table out and stick it to your multi-meter case or workshop wall for handy future reference.

A simple calculator to do all these combinations is available here.

Congratulations on having finished reading these first two articles about electrical fundamentals.. It has been very heavy with theory and all sorts of formulas, but now you have the basics to understand most electrical and electronic principles.




  1. Hi Geoff,

    Nice article and easy to understand.

    I thought I would cement the knowledge with a bit of practical application, so grabbed a 240 V/100 Watt lightbulb and my trusty DMM. I plugged the voltage and wattage into the calculator and it seems to me that the bulb would draw .42 Amps and would have a resistance of 576 Ohms. Now here is the part that is confusing me, when I set my DMM on the 200 Ohm setting and measure the resistance, the meter tells me that the resistance is only 40.6 Ohms. Did I do something incorrectly, or is there some other explanation for this apparent discrepancy?

    • Hi Josh,

      Your calcs and assumption are basically correct. What you are missing is that resistance increases with temperature You were measuring the cold filament resistance. When you turn the light on, the filament temperature rises to really really hot. And the resistance increases accordingly – to around 576 ohms I would guess.

      Hopefully that helps explain your conundrum. The other issue that can come into play is impedance in an AC circuit. This is especially relevant with a coil, like in a heater or speaker coil. Then your DMM will only measure the DC resistance, not the AC impedance which also varies with frequency – significant with speakers.

      Hope this helps


  2. I get the underlying theory of ohms watts etc. There is one point where i get confused and i was hoping you could provide clarity.

    Say you are installing 8 JBL SRX812, which have one 8 ohm speaker in each at a church. Power Handling: 3200W Peak, 1600W Program, 800W Continuous. Typically people recommend choosing an amplifier that is slightly above the program rating and not above the peak amount. Additionally, i am under the impression that being below the continuous rating would be bad and underpower the speaker.

    So when choosing an amp with the scenario i created i would be looking for an amplifier that does 1600-3200 watts @ 2 ohms. I chose 2 ohms because i will daisy chain 4 speakers per amp channel. 8ohms/4spkr = 2ohms. So an XTI4002 does 1600 @ 2 ohms and XTI6002 does 3000 @ 2 ohms.

    XTI 4002 2 ohm 1600 4 ohm 1200 8 ohm 650

    Now for the confusing part. It almost feels like inverse logic to say that if we add more speakers to the chain we get MORE power from the amplifier. Then you look at ohms law and realize this could actually make sense because resistance going down (by adding more speakers which feel weird) means that wattage will go up.

    So my main question is related to how that wattage is distributed? If i used an xti4002 to power one of these speakers on an amp channel, the amp would give 650 watts @ 8 ohms which is below the continuous and underpowering the speaker. If i now run 2 speakers on that one channel, the ohms are down to 4 and the amp will deliver 1200 watts so we are good but not great. We are above the continuous but below the program power. But wait, now their are two speakers… So does that really mean that 600 watts goes to each speaker? So we are still screwed and underpowering the speaker or am i just confused?

    Hopefully this was clear on the confusing part of the practical application of picking amps and speakers that make sense for a system. Look forward to hearing a response.


    • Hi Rob,

      I think you have it.

      Your maths and understanding are correct. Lowering the total impedance increase the current which increases the wattage, up to the point where the amp can not deliver any more.

      Your summary of having the power of an amp above the RMS rating of the speaker but below the peak is reasonable. However, as the speaker manufactures constantly say: it doesn’t matter what size amp you have, if you try hard enough you can always blow a speaker. In some cases, you can drive the church with 50 watts or 5000 watts per speaker and it will be fine, but don’t run it so loud that you come even close to distortion (distortion being an early warning sign of impending damage).

      So don’t get too hung up about having to comply to a tight criteria for amp/speaker matching. Work out how loud you need it to go, and then calculate the wattage you need for a particular speaker. This calculator might help.

      You are also correct in the last paragraph in saying the power from an amp is divided by the number of speakers connected in parallel to it.

      Personally, my approach would be to first estimate the wattage required (using something like the above mentioned calculator). Then I would normally design it so that there are a maximum of two speakers in parallel on any one amp. This has a number of advantages. It means if an amp dies, you don’t lose half your speakers, it allows you to use amps which only need to work down to 4 ohms, and it allows each pair of speakers to have different EQ or time delay as and if required. The price of then extra amps is a bit offset by not having to have such powerful amps into 2 ohms.

      Hope this help some



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