A power station is a place where other forms of energy - coal, gas, potential energy in water and nuclear energy - are turned into electrical energy for transmission to places that use electrical energy. Electrical engineering is concerned with transmission and ultilization of two things - energy and information. Here, in this lesson, we are going to focus on power and energy. In this lesson you will want to learn the following.
Given an electrical circuit or device
Be able to compute instantaneous rate of energy use (power).
What Is Electrical Power?
Electrical power is conceptually simple. Consider a device that has a voltage across it and a current flowing through it. That situation is shown in the diagram at the right.
- The voltage across the device is a measure of the energy - in joules - that a unit charge - one couloumb - will dissipate when it flows through the device. (Click here to go to the lesson on voltage if you want to review.) If the device is a resistor, then the energy will appear as heat energy in the resistor. If the device is a battery, then the energy will be stored in the battery.
- The current is the number of couloumbs that flows through the device in one second.j (Click here to go to the lesson on current if you want to review.)
- If each couloumb dissipates V joules, and I couloumbs flows in one second, then the rate of energy dissipation is the product, VI.
- It doesn't matter what the electrical device is, the rate at which energy is delivered to the device is VI as long as the voltage and current are defined as shown.
- The power can be negative. If the device is a battery, then current - as defined in the figure - can easily be negative if, for example, a resistor is attached to the battery. If the power is negative, then the rate at which the device expends energy is negative. That really means that it is delivering energy in that situation.
Power in Electrical Devices A resistor is one device for which you can compute power dissipation.
- A symbol for a resistor is shown below, along with a voltage, Vr, across the resistor and a current, Ir, flowing through the resistor.
- We can compute the power delivered to the resistor. It's just the product of the voltage across the resistor and the current through the resistor, VrIr.
- In a resistor, there is a relationship between the voltage and the current, and we can use that knowledge to get a different expression - one that will give more insight.
- We know that Vr = Rir, so the power is just:
- Power into the resistor = VrIr = (RIr)Ir = R(Ir)2.
- We can also use the expression for the current Ir = Vr/R,
- Power into the resistor = VrIr = Vr(Vr/R) = (Vr)2/R.
- The power dissipated by a resistor is always positive. That means that it does not (and in fact it could not) generate energy. It always dissipates energy - uses it up - contributing to the heat death of the universe.
- We know the power is positive because R is always positive (and it will always be for any resistor that doesn't have hidden transistors) and because the square of the current has to be a positive number.
ProblemsP1. You have a 1KW resistor, and there is 25 volts across the resistor. Determine the power (in watts) that the resistor dissipates.
P2. You have a 25 watt light bulb that operates with 12.6 volts across it. Determine the resistance of the light bulb.
Power In Batteries Batteries are ubiquitous components. They are in TV remotes, cell phones and things like that. But, batteries also appear in places you don't expect them to be. For example, you can turn this computer off. When you turn it back on it remembers things and recalculates things like the time. Now, you expect that for things that can be stored on a hard drive. You don't expect it for the time.
When you turn this computer off and later turn it back on it will have the right date and time. How does it do that? If you think about it (and don't do that for too long!) you have to believe that there is a battery somewhere inside the computer and that when you turn the computer off that battery runs some sort of little clock hidden inside the computer. You can't see the clock and you wouldn't even know it's there, but you can probably see the time now on the task bar of this computer - and it's probably close to being right!
Batteries are used to solve many problems.
- They are used to provide power to run things like computer clocks that need to keep running even in the absence of AC power.
- They are used to store energy for things like starting a car. When you run the car you generate energy (from the gasoline) and store it in the car battery. Then there is energy there when you need it to get the car going again.
- They are used for low power devices to make them portable. That includes things like cell phones, TV remotes and calculators.
- There is energy stored in the battery and the battery delivers stored energy to the resistor.
- The resistor dissipates energy, and what happens physically is that the electrical energy that is delivered to the resistor gets turned into heat energy and the resistor becomes warmer.
- In the diagram, we have defined a battery voltage, Vb, and a current, Ir.
- Notice that we have used a natural definition for the current polarity. We have the arrow pointing out of the battery and into the resistor. We do that because we know that positive charge actually flows from the battery terminal through the resistor.
- That definition of current polarity raises questions about calculation of power to/from the battery. Let us consider the power flow into the battery.
Power flow into the battery or any other device - is the product, VI, when
- V is the voltage across the device, and
- I is the current flowing into the device.
- Remember, for our polarity conventions here, the current arrow points into the terminal of the device that is labelled "+" for the voltage definition.
- The power flowing into the battery is negative!
- The power flowing out of the battery is positive!
- And, it makes sense because we know the battery supplies power.
- Batteries are often rated in ampere-hours (or milliampere-hours) and an ampere-hour is really a unit of charge.
- As a battery is used it discharges - charge flows from the battery - but it tends to hold a constant voltage. This is different than the internal resistance of the battery. What we are saying here is that as time goes on - for the same current drawn from the battery - the voltage stays about the same. There may be a slight drop-off but it is not very large.
- Thus, if we have a 12.6 v battery, it will have something close to 12.6v until it gets close to being discharged.
- Let's say we have a 12.6v battery rated at 70 ampere-hours.
- Assuming it can deliver 1 ampere for 70 hours, then it will be delivering
- Power = 12.6v x 1.0 amp = 12.6 watts for 70 hours.
- That works out to 12.6 x 70 = 882 watt hours or .882 kw-hr. - and remember you pay the
- electric company by the kilowatt-hour!
- In joules we have 882 w-hr x 3600sec/hr = 3,175,200 joules.
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