Question

Difficulty: MediumConduction of Electricity Through Gases and Cathode Rays

In a cathode-ray experiment, a beam of electrons passes undeflected through mutually perpendicular electric and magnetic fields. If the electric field intensity is 4.0×104 V m14.0 \times 10^4\text{ V m}^{-1} and the magnetic flux density is 2.0×103 T2.0 \times 10^{-3}\text{ T}, what is the speed of the electrons in the beam?

  1. 2.0×107 m s12.0 \times 10^7\text{ m s}^{-1}Answer
  2. B
    8.0×101 m s18.0 \times 10^1\text{ m s}^{-1}
  3. C
    5.0×108 m s15.0 \times 10^{-8}\text{ m s}^{-1}
  4. D
    2.0×101 m s12.0 \times 10^1\text{ m s}^{-1}

Answer

The speed of the electrons in the beam is 2.0×107 m s12.0 \times 10^7\text{ m s}^{-1}.
When a cathode ray beam passes undeflected through perpendicular electric (EE) and magnetic (BB) fields, the electric force (eEeE) and magnetic force (evBevB) are equal in magnitude and opposite in direction. Equating eE=evBeE = evB simplifies to v=EBv = \frac{E}{B}. Substituting E=4.0×104 V m1E = 4.0 \times 10^4\text{ V m}^{-1} and B=2.0×103 TB = 2.0 \times 10^{-3}\text{ T} yields an electron speed of 2.0×107 m s12.0 \times 10^7\text{ m s}^{-1}.

Step-by-Step Solution

1
Identify the condition for no deflection in crossed electric and magnetic fields.
The electrostatic force Fe=eEF_e = eE equals the magnetic force Fb=evBF_b = evB.
For zero net deflection, the opposing electric and magnetic forces must balance each other exactly.
2
Rearrange the force balance equation to solve for speed vv.
v=EBv = \frac{E}{B}
Canceling the charge ee on both sides of eE=evBeE = evB isolates velocity vv as the ratio of electric field to magnetic field.
3
Substitute the given values into the velocity equation.
v=4.0×104 V m12.0×103 T=2.0×107 m s1v = \frac{4.0 \times 10^4\text{ V m}^{-1}}{2.0 \times 10^{-3}\text{ T}} = 2.0 \times 10^7\text{ m s}^{-1}
Evaluating 4.02.0×104(3)\frac{4.0}{2.0} \times 10^{4 - (-3)} gives 2.0×107 m s12.0 \times 10^7\text{ m s}^{-1}.

Key Concept

Velocity selector condition for cathode rays in crossed electric and magnetic fields
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