explain how electric and magnetic fields can be used in velocity selection

Force on a Current-Carrying Conductor

When a conductor carrying an electric current $I$ is placed in a magnetic field $\\mathbf{B}$, it experiences a magnetic force. The force is given by the cross‑product:

$$\\mathbf{F}=I\\,\\mathbf{L}\\times\\mathbf{B}$$

Here $\\mathbf{L}$ is the vector that points along the length of the conductor, its magnitude being the length $L$. The direction of $\\mathbf{F}$ follows the right‑hand rule: point your fingers in the direction of $\\mathbf{L}$, curl them toward $\\mathbf{B}$, and your thumb points in the direction of the force.

Analogy: A Boat in a River

  • ⚓️ Current is like the boat’s engine pushing it forward.
  • 🌊 Magnetic field is like the river’s current pushing sideways.
  • 🚤 The force on the boat is the combined effect of its engine and the river, giving it a new direction.

Why Does the Force Matter?

In devices such as electric motors, the magnetic force turns the rotor. In particle detectors, it bends the path of charged particles, allowing us to measure their properties.

Velocity Selection Using Electric and Magnetic Fields

Charged particles moving through perpendicular electric $\\mathbf{E}$ and magnetic $\\mathbf{B}$ fields can be filtered by their velocity. The key idea is to balance the electric and magnetic forces so that only particles with a specific speed pass straight through.

Force Balance Condition

The electric force is $\\mathbf{F}_E=q\\,\\mathbf{E}$ and the magnetic force is $\\mathbf{F}_B=q\\,\\mathbf{v}\\times\\mathbf{B}$. For a particle to travel undeflected, these forces must cancel:

$$q\\,\\mathbf{E}=q\\,\\mathbf{v}\\times\\mathbf{B}$$

Assuming $\\mathbf{E}$ and $\\mathbf{B}$ are perpendicular and the velocity $\\mathbf{v}$ is along the conductor, we get the simple relation:

$$v=\\frac{E}{B}$$

Only particles with speed $v$ will go straight; others will be deflected.

Practical Example: The Velocity Selector in a Mass Spectrometer

  1. ⚡️ An electric field $E$ is applied horizontally.
  2. 🧲 A magnetic field $B$ is applied vertically.
  3. 🚀 Ions from a source enter the region with a velocity $v$.
  4. Only ions satisfying $v=E/B$ pass straight through to the detector.

Table: Force Comparison for Different Velocities

Velocity $v$ Electric Force $F_E$ Magnetic Force $F_B$ Resulting Path
$v = E/B$ $qE$ $qE$ Straight line 🚶‍♂️
$v > E/B$ $qE$ $>qE$ Deflected left 🔄
$v < E/B$ $qE$ $ Deflected right 🔄

Key Takeaways

  • ⚡️ The magnetic force on a current-carrying wire is proportional to current, length, and magnetic field strength.
  • 🧲 The direction follows the right‑hand rule.
  • 🚀 By balancing electric and magnetic forces, we can select particles of a particular velocity.
  • 🔬 This principle is the basis of many instruments, from electric motors to mass spectrometers.

Revision

Log in to practice.

10 views 0 suggestions