Chapter 22 : Electric potential

Presentation on theme: "Chapter 22 : Electric potential"— Presentation transcript:

1 Chapter 22 : Electric potential
What is electric potential? How does it relate to potential energy? How does it relate to electric field? Some simple applications

2 Electric potential What does it mean when it says “1.5 Volts” on the battery? The electric potential difference between the ends is 1.5 Volts

3 Electric potential 1.5 V 230 V 100,000 V So what is a volt?

4 Electric potential 𝑊=𝑞×∆𝑉
The electric potential difference ∆𝑉 in volts between two points is the work in Joules needed to move 1 C of charge between those points ∆𝑉 is measured in volts [V] : 1 V = 1 J/C 𝑊=𝑞×∆𝑉 W = work done [in J] q = charge [in C] ∆V = potential difference [in V]

5 Electric potential 𝑊=𝑞×∆𝑉
The electric potential difference ∆𝑉 in volts between two points is the work in Joules needed to move 1 C of charge between those points 𝑊=𝑞×∆𝑉 The 1.5 V battery does 1.5 J of work for every 1 C of charge flowing round the circuit

6 Potential energy What is this thing called “potential”?
Potential energy crops up everywhere in physics

7 Potential energy 𝐹=𝑚𝑔 𝑊=𝐹×ℎ 𝐹 =𝑚𝑔ℎ ℎ →𝑈=𝑚𝑔ℎ
Potential energy U is the energy stored in a system (when work is done against a force) e.g. force of gravity … 𝐹=𝑚𝑔 Work = Force x Distance 𝑊=𝐹×ℎ 𝐹 =𝑚𝑔ℎ ℎ →𝑈=𝑚𝑔ℎ

8 Potential energy Potential energy may be released and converted into other forms (such as kinetic energy) Work is done, increasing the potential energy

9 Potential energy Potential energy difference is the only thing that matters – not the reference (or zero) level For example, applying conservation of energy to a mechanics problem: Final energy = Initial energy 𝐾𝐸 𝑓𝑖𝑛𝑎𝑙 + 𝑃𝐸 𝑓𝑖𝑛𝑎𝑙 = 𝐾𝐸 𝑖𝑛𝑖𝑡𝑖𝑎𝑙 + 𝑃𝐸 𝑖𝑛𝑖𝑡𝑖𝑎𝑙 𝐾𝐸 𝑓𝑖𝑛𝑎𝑙 = 𝐾𝐸 𝑖𝑛𝑖𝑡𝑖𝑎𝑙 + (𝑃𝐸 𝑖𝑛𝑖𝑡𝑖𝑎𝑙 − 𝑃𝐸 𝑓𝑖𝑛𝑎𝑙 ) Difference in potential energy

10 Potential energy Potential energy difference doesn’t depend on the path – only on the two points A and B

11 Potential energy 𝐹=𝑘𝑥 𝐹 𝑊= 𝑘𝑥 𝑑𝑥 = 1 2 𝑘 𝑥 2 →𝑈= 1 2 𝑘 𝑥 2 𝑥
Potential energy U is the energy stored in a system – second example e.g. stretching a spring … 𝐹=𝑘𝑥 Work = Force x Distance Force is varying with distance! 𝐹 𝑊= 𝑘𝑥 𝑑𝑥 = 𝑘 𝑥 2 𝑥 →𝑈= 𝑘 𝑥 2

12 Electric potential 𝐹 𝐹=−𝑞𝐸 𝐸 𝑊=𝐹 ∆𝑥 =−𝑞𝐸 ∆𝑥 𝐸=− ∆𝑉 ∆𝑥
e.g. moving a charge through an electric field… 𝐹 𝐹=−𝑞𝐸 𝑞 𝐸 (minus sign because the force is opposite to E) ∆𝑥 Work = Force x Distance 𝑊=𝐹 ∆𝑥 =−𝑞𝐸 ∆𝑥 Potential difference ∆𝑉 is work needed to move 1C of charge: 𝑊=𝑞 ∆𝑉 Equate: 𝑞 ∆𝑉=−𝑞𝐸 ∆𝑥 𝐸=− ∆𝑉 ∆𝑥

13 Electric potential 𝑉 𝐸 𝑥 𝑥
Electric field is the gradient of potential 𝐸=− ∆𝑉 ∆𝑥 High V Low V 𝑉 𝐸 𝑥 Positive charges feel a force from high to low potential Negative charges feel a force from low to high potential 𝑥

14 Two parallel plates have equal and opposite charge
Two parallel plates have equal and opposite charge. Rank the indicated positions from highest to lowest electric potential. • A • • B D • C A=C, B=D A, B, C, D C, D=B, A A, B=D, C

15 Electric potential 𝑉 𝑥 Analogy with gravitational potential
Gravitational potential difference exerts force on mass 𝑉 𝑞 Electric potential difference exerts force on charge 𝑥

16 Electric potential Electric field is the gradient of potential 𝐸=− ∆𝑉 ∆𝑥 High V Low V The dashed lines are called equipotentials (lines of constant V) Electric field lines are perpendicular to equipotentials It takes no work to move a charge along an equipotential (work done = 𝑑𝑊= 𝐹 . 𝑑𝑥 =𝑞 𝐸 . 𝑑𝑥 =0) 𝐸

17 Electric potential Summary for two plates at potential difference V 𝐸 Electric field is the potential gradient Work W to move charge q from –ve to +ve plate 𝐸= 𝑉 𝑑 𝑊=𝑞 𝑉 𝑑

18 Link to potential energy
The electric potential difference ∆𝑉 between two points is the work needed to move 1 C of charge between those points This work is also equal to the potential energy difference ∆𝑈 between those points Potential V = potential energy per unit charge U/q 𝑊=𝑞×∆𝑉 ∆𝑈=𝑞×∆𝑉

19 • • • • • - - - - - - - - - - - - - A B C D A or C C or D
An electron is placed at “X” on the negative plate of a pair of charged parallel plates. For the maximum work to be done on it, which point should it be moved to? • • X D • B • A • C A B C D A or C C or D

20 Electric potential What is the electric potential near a charge +Q? Work = Force x Distance 𝐹= 𝑘 𝑄 𝑞 𝑥 2 Force is varying with distance, need integral! 𝑊= ∞ 𝑟 𝐹 𝑑𝑥 = ∞ 𝑟 − 𝑘 𝑄 𝑞 𝑥 2 𝑑𝑥 = 𝑘 𝑄 𝑞 𝑟 +q Potential energy 𝑈= 𝑘 𝑄 𝑞 𝑟 𝑥 +Q + Electric potential 𝑉= 𝑈 𝑞 = 𝑘 𝑄 𝑟

21 Electric potential What is the electric potential near a charge +Q? +q 𝑟 +Q + Electric potential 𝑉= 𝑘 𝑄 𝑟

22 Electric potential Exercise: a potential difference of 200 V is applied across a pair of parallel plates m apart. (a) calculate E and draw its direction between the plates. The electric field is the gradient in potential 𝐸= ∆𝑉 ∆𝑥 = =1.7× 𝑉 𝑚 −1 [𝑜𝑟 𝑁 𝐶 −1 ] 𝑉=200 +ve plate 𝐸 𝑉=0 -ve plate

23 Electric potential 𝐸 −𝑒
Exercise: a potential difference of 200 V is applied across a pair of parallel plates m apart. (b) an electron is placed between the plates, next to the negative plate. Calculate the force on the electron, the acceleration of the electron, and the time it takes to reach the other plate. Force 𝐹=𝑞𝐸 =(−1.6× 10 −19 )×(1.7× 10 4 ) =−2.7× 10 −15 𝑁 Acceleration 𝑎= 𝐹 𝑚 = 2.7× 10 − × 10 −31 𝐹=𝑚𝑎 =3.0× 𝑚 𝑠 −2 +ve plate Time 𝑡= 2𝑑 𝑎 𝑑= 𝑎 𝑡 2 𝐸 −𝑒 𝑡= 2× × 10 15 =2.8× 10 −9 𝑠 -ve plate e = 1.6 x C; me = 9.1 x kg

24 Electric potential 𝐸 −𝑒
Exercise: a potential difference of 200 V is applied across a pair of parallel plates m apart. (c) calculate the work done on the electron as it travels between the plates. The potential difference is the work done on 1C charge Work 𝑊=𝑞𝑉 = 1.6× 10 −19 ×200 =3.2× 10 −17 𝐽 +ve plate 𝐸 −𝑒 -ve plate e = 1.6 x C; me = 9.1 x kg

25 Chapter 22 summary Electric potential difference V is the work done when moving unit charge: 𝑊=𝑞𝑉 The electric potential energy is therefore also given by: 𝑈=𝑞𝑉 The electric field is the gradient of the potential: 𝐸=−∆𝑉/∆𝑥 Charges feel a force from high electric potential to low potential