Charged Particles in a Velocity Selector
- A velocity selector is defined as:
A device consisting of perpendicular electric and magnetic fields where charged particles with a specific velocity can be filtered
- Velocity selectors are used in devices, such as mass spectrometers, in order to produce a beam of charged particles all travelling at the same velocity
- The construction of a velocity selector consists of two horizontal oppositely charged plates situated in a vacuum chamber
- The plates provide a uniform electric field with strength E between them
- There is also a uniform magnetic field with flux density B applied perpendicular to the electric field
- If a beam of charged particles enter between the plates, they may all have the same charge but travel at different speeds v
- The electric force does not depend on the velocity: FE = EQ
- However, the magnetic force does depend on the velocity: FB = BQv
- The magnetic force will be greater for particles which are travelling faster
- To select particles travelling at exactly the desired the speed v, the electric and magnetic force must therefore be equal, but in opposite directions
FE = FB
The particles travelling at the desired speed v will travel through undeflected due to the equal and opposite electric and magnetic forces on them
- The resultant force on the particles at speed v will be zero, so they will remain undeflected and pass straight through between the plates
- By equating the electric and magnetic force equations:
EQ = BQv
- The charge Q will cancel out on both sides to give the selected velocity v equation:
- Therefore, the speed v in which a particle will remain undeflected is found by the ratio of the electric and magnetic field strength
- If a particle has a speed greater or less than v, the magnetic force will deflect it and collide with one of the charged plates
- This would remove the particles in the beam that are not exactly at speed v
- Note: the gravitational force on the charged particles will be negligible compared to the electric and magnetic forces and therefore can be ignored in these calculations
Worked example
A positive ion travels between two charged plates towards a slit S.
Part (a)
Step 1: Determine the direction of the E field
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- Electric field lines point from the positive to negative to charge
- Therefore, it must be directed vertically upwards
Step 2: Determine the direction of the B field
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- Using Fleming’s left-hand rule:
- The charge or current I is directed to the right
- B must be directed out of the page / screen for the magnetic force F to act vertically downwards
- Using Fleming’s left-hand rule:
Part (b)
Step 1: List the known quantities
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- Electric field strength, E = 2.8 kV m−1 = 2.8 × 103 V m−1
- Magnetic flux density, B = 0.50 T
Step 2: Write down the velocity selector equation
Step 3: Calculate the speed of the ion at S
= 5600 m s−1
Part (c)
Step 1: Consider the effect of changing the ion's speed on the electric and magnetic forces
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- Electric force is given by:
FE = EQ
-
- Therefore, electric force does not depend on the velocity
- Magnetic force is given by:
FB = BQv
-
- Therefore, FB ∝ v, so if the speed increases, the magnetic force must increase
Step 2: Determine the net direction of the force
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- Since the net magnetic force would direct the ion downwards in the direction of the field
- The ion will be deflected towards the positive plate