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Electric Potential (HL) (HL IB Physics)

Revision Note

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Ann H

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Ann H

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Electric Potential

  • In order to move a positive charge closer to another positive charge, work must be done to overcome the force of repulsion between them
  • Energy is therefore transferred to the charge that is being pushed upon
    • This means its potential energy increases

  • If the positive charge is free to move, it will start to move away from the repelling charge
    • As a result, its potential energy decreases back to 0

  • This is analogous to the gravitational potential energy of a mass increasing as it is being lift upwards and decreasing and it falls
  • The electric potential at a point is defined as:

The work done per unit positive charge in bringing a small test charge from infinity to a defined point

  • Electric potential is a scalar quantity
    • This means it doesn’t have a direction
  • However, you will still see the electric potential with a positive or negative sign. This is because the electric potential is:
    • Positive when near an isolated positive charge
    • Negative when near an isolated negative charges
    • Zero at infinity

  • Positive work is done by the mass from infinity to a point around a positive charge and negative work is done around a negative charge. This means:
    • When a test charge moves closer to a negative charge, its electric potential decreases
    • When a test charge moves closer to a positive charge, its electric potential increases

  • To find the potential at a point caused by multiple charges, add up each potential separately

Calculating Electric Potential

  • The electric potential in the field due to a point charge is defined as:

 

bold italic V subscript bold e bold space bold equals bold space fraction numerator bold Q over denominator bold 4 bold pi bold epsilon subscript bold 0 bold r end fraction

  • Where:
    • Ve = the electric potential (V)
    • Q = the point charge producing the potential (C)
    • ε0 = permittivity of free space (F m-1)
    • r = distance from the centre of the point charge (m)

  • This equation shows that for a positive (+) charge:
    • As the distance from the charge r decreases, the potential Ve increases
    • This is because more work has to be done on a positive test charge to overcome the repulsive force

  • For a negative (−) charge:
    • As the distance from the charge r decreases, the potential Ve decreases
    • This is because less work has to be done on a positive test charge since the attractive force will make it easier

  • Unlike the gravitational potential equation, the minus sign in the electric potential equation will be included in the charge
  • The electric potential changes according to an inverse square law with distance

Potential around charged sphere, downloadable AS & A Level Physics revision notes

The potential changes as an inverse law with distance near a charged sphere

  • Note: this equation still applies to a conducting sphere. The charge on the sphere is treated as if it concentrated at a point in the sphere from the point charge approximation

Worked example

A Van de Graaf generator has a spherical dome of radius 15 cm. It is charged up to a potential of 240 kV. Calculate

(a) How much charge is stored on the dome

(b) The potential a distance of 30 cm from the dome

Answer:

Part (a)

Step 1: List down the known quantities

  • Radius of the dome, r = 15 cm = 15 × 10-2 m
  • Potential difference, V = 240 kV = 240 × 103 V

Step 2: Write down the equation for the electric potential due to a point charge

Electric Potential Due to a Point Charge equation

Step 3: Rearrange for charge Q

Q = V4πε0r

Step 4: Substitute in values

Q = (240 × 103) × (4π × 8.85 × 10-12) × (15 × 10-2) = 4.0 × 10-6 C = 4.0 μC

Part (b)

 Step 1: Write down the known quantities

  • Q = charge stored in the dome = 4.0 μC = 4.0 × 10-6 C
  • r = radius of the dome + distance from the dome = 15 + 30 = 45 cm = 45 × 10-2 m

Step 2: Write down the equation for electric potential due to a point charge

Electric Potential Due to a Point Charge equation

Step 3: Substitute in values

Electric Potential Due to a Point Charge Worked Example equation

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Ann H

Author: Ann H

Ann obtained her Maths and Physics degree from the University of Bath before completing her PGCE in Science and Maths teaching. She spent ten years teaching Maths and Physics to wonderful students from all around the world whilst living in China, Ethiopia and Nepal. Now based in beautiful Devon she is thrilled to be creating awesome Physics resources to make Physics more accessible and understandable for all students no matter their schooling or background.