1. Electric Potential Energy and Electric Potential DifferencePg

2. Electric Fields
From the definition of an electric field as a force acting on a charge, it follows that, for a given uniform electric field, charge, and particle mass, the particles undergoes a uniform acceleration (since the force is constant)
This ability of an electric field to accelerate charged particles with known conditions has proven useful to physicists and engineers

3. Electric Fields & Particle Acceleration
For example, particle accelerators are used to accelerate particles to speeds near the speed of light
They are also used in a large variety of other application including particle therapy for oncological purposes

4. Electric Fields & Particle Acceleration
Particle acceleration is also important in some everyday devices as well
For example, ink droplets from the print head of an inkjet printer are either charged or uncharged
The uncharged droplets move to the paper undeflected, forming the letters
Charged droplets are deflected into the gutter, leaving those parts of the paper blank

5. Electric Fields & Particle Acceleration
Another application of particle acceleration is old television sets and computer monitors which have cathode-ray tubes
These tubes acceleration electrons towards a phosphor screen
Variations in the deflection of the accelerated electrons determine the brightness and colour of the screen

6. Work & Electric Fields
Recall that in a region of space where the electric field is constant, has the same magnitude and direction at all points
A point charge, q, in this region experiences an electric force FE = q that is parallel to

7. Work & Electric Fields
Suppose this charge moves a certain distance, d, starting at point A and ending at point B
If we assume the displacement is parallel to the electric force, then the work done by the electric force on the charge is:
Note: the electric force does work on the charge and is independent of the path it takes from A to B

8. Work & Potential Energy
We can now define the electric potential energy, EE, which is the energy stored in the system that can do work, W, on a positively charged particle
From your studies you know that the charge in the potential energy associated with this type of force is equal to –W (i.e. the electric field has lost energy doing work on the particle to accelerate it)

9. Work & Electric Potential Energy
So, if the electric force does an amount of work, W, on a charged particle, the change in the electric potential energy is:
The change in the potential energy depends on the starting and ending location but not the path taken

10. Electric Potential Energy Difference

11. Electric Potential Energy Difference
For example, if a positive charge, q, is moved from A to B, against the electric field, by an external force, then the work done by the electric field on the particle is negative
In other words, a positive amount of energy is stored in the system, composed of the charge, q, and the electric field (i.e. ∆EE > 0)
This energy loss could appear as a decrease in the kinetic energy of the particle

12. Practice 1. A charged particle moves in a uniform electric field
A) For a proton (q = +1/6 x C), calculate the change in potential energy when the magnitude of the electric field is 250 N/C [E], the starting position is 2.4 mm from the origin, and the final position is 3.9 m from the origin
B) Calculate the change in the electric potential eneryg for an electron (q = -1.6 x C) in the same field and with the same displacement
2. Using the law of conservatino of energy, calculate the final speed of the proton (m = 1.67 x kg) in part (a) of question 1 for the given displacement. Assume that the proton starts from rest.

13. Practice
3. Determine the initial speed of the electron (m = x kg) in part (b) of question 1, assuming it has come to rest after the same displacement.
Textbook page 349, #1-3

14. Electric Potential
As discussed earlier, the electric potential energy is not the property of a single charge alone – it depends on the value of the charge(s) and the electric field involved
This leads to a new quantity called electric potential, V, which is a measure of how much electric potential energy is associated with a specific quantity of charge at a particular location in an electric field
Based on this definition:

15. Electric Potential (V)
The value of potential energy per unit positive charge for a given point in an electric field (1V = 1 J/C = 1 N-m/C)
Electric potential, or just potential, is a convenient measure because it is independent of the amount of charge at a particular location in the field
It depends only on the electric field strength at that location
For example, if you had 1 C of electrons at a particular location in a uniform electric field, you would possess X J of electric potential energy
If you doubled the amount of electrons to 2 C at the same location in the electric field, you would have 2X J of electric potential energy
In both situations, however, you would have the same electric potential (V = XJ/1C = 2XJ/2C = XJ/C)

16. Electric Potential Difference
Another convenient definition relating to electric potential energy is electric potential difference, ∆V.
We can define the change in the potential, or the potential difference, for a charge q that moves between two points as:
**this is the same potential difference you talked about in both grades 9 and 11…….just a more formal definition
**recall that the electric potential difference between two points in a circuit is measured with a voltmeter connected in parallel to the path of moving charges

17. Electric Potential Difference
The electric potential difference (∆V) is the amount of work required per unit charge to move a positive charge from one point to another in the presence of an electric field

18. Electric Potential Difference
For the case of a uniform electric field, the equation for electric potential difference becomes:

19. Electric Potential Difference (∆V)
The amount of work required per unit charge to move a positive charge from one point to another in the presence of an electric field

20. Electric Potential Difference
Now, rearranging for (the electric field intensity) we get the following relationship:
Notice that this relationship shows how a non-uniform electric field varies with the change in electric potential (electric potential difference) and the change in position in the field

21. Electric Potential Difference
According to the equation, the electric field
Is largest in regions where V is large
Changes rapidly with small changes in displacement
Is zero in regions where V is constant
Points from regions of high potential to regions of low potential

22. Electric Potential Difference
If we consider a circuit in which a battery is the source of electrical energy, a positive test charge will naturally move in the same direction as the electric field from the positive terminal where a high potential exists to the negative terminal where a low potential exists – conventional current
Conversely, electrons will naturally travel from a region of low potential to a region of high potential, in a direction opposite to the direction of the electric field – electron flow

23. Practice

24. Textbook
Pg. 349, #1-3
Pg. 354, #2, 3