11- Magnetic field and moving charges

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1
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What is the Lorentz Force?

The force exerted on a moving charge by a magnetic field,

  • q is the charge

  • v⃗ is velocity

  • B⃗ is the magnetic field.

<p>The force exerted on a moving charge by a magnetic field,</p><p></p><ul><li><p><strong>q</strong> is the charge</p></li><li><p><strong>v⃗</strong> is velocity</p></li><li><p><strong>B⃗</strong> is the magnetic field.</p></li></ul><p></p>
2
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How is the direction of the Lorentz force determined?

By the right-hand rule:

  • Thumb points in direction of v⃗ × B⃗

  • If q is positive, F⃗ is in the same direction as v⃗ × B⃗

  • If q is negative, F⃗ is in the opposite direction

<p>By the right-hand rule:</p><ul><li><p class="">Thumb points in direction of <strong>v⃗ × B⃗</strong></p></li><li><p class="">If <strong>q</strong> is positive, <strong>F⃗</strong> is in the same direction as <strong>v⃗ × B⃗</strong></p></li><li><p class="">If <strong>q</strong> is negative, <strong>F⃗</strong> is in the opposite direction</p></li></ul><p></p>
3
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Why can't the Lorentz force change a particle’s speed?

Because it is always perpendicular to velocity v⃗, meaning it cannot do work or change kinetic energy—only the direction of motion.

<p>Because it is always perpendicular to velocity <strong>v⃗</strong>, meaning it cannot do work or change kinetic energy—only the direction of motion.</p>
4
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What is a Hall Probe?

  • A device that measures magnetic fields using the Hall effect

  • A voltage difference (Hall voltage, VH) is generated due to charge deflection by a magnetic field.

<ul><li><p>A device that measures magnetic fields using the Hall effect</p></li></ul><p></p><ul><li><p>A voltage difference (Hall voltage, <strong>V<sub>H</sub></strong>) is generated due to charge deflection by a magnetic field.</p></li></ul><p></p>
5
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How does a Hall Probe work?

  • A current I flows through a semiconductor slab placed perpendicular to B⃗.

  • The Lorentz force deflects charge carriers, creating a charge separation and an internal electric field E⃗H that balances the force.

<ul><li><p>A current <strong>I</strong> flows through a semiconductor slab placed perpendicular to <strong>B⃗</strong>. </p></li></ul><p></p><ul><li><p>The Lorentz force deflects charge carriers, creating a charge separation and an internal electric field <strong>E⃗<sub>H</sub></strong> that balances the force.</p></li></ul><p></p>
6
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<p>What is the Hall voltage equation?</p>

What is the Hall voltage equation?

  • kH = Hall coefficient (material-dependent)

  • I = Current through the sample

  • B = Magnetic field strength

<ul><li><p class=""><strong>k<sub>H</sub></strong> = Hall coefficient (material-dependent)</p></li><li><p class=""><strong>I</strong> = Current through the sample</p></li><li><p class=""><strong>B</strong> = Magnetic field strength</p></li></ul><p></p>
7
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What is the force on a charge in simultaneous electric and magnetic fields?

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8
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How can the net force on a charge be zero in combined E⃗ and B⃗ fields?

If E⃗ and B⃗ are perpendicular, the charge moves at a velocity v where electric and magnetic forces cancel, leading to F⃗ = 0.

<p>If <strong>E⃗</strong> and <strong>B⃗</strong> are perpendicular, the charge moves at a velocity <strong>v</strong> where electric and magnetic forces cancel, leading to <strong>F⃗ = 0</strong>.</p>
9
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What experimental setup did J.J. Thomson use to discover the electron?

  • A cathode ray tube with a beam of charged particles passing through crossed electric (E⃗) and magnetic (B⃗) fields

  • This allowed him to control and measure their deflection.

<ul><li><p>A <strong>cathode ray tube</strong> with a beam of charged particles passing through <strong>crossed electric (E⃗) and magnetic (B⃗) fields</strong></p></li></ul><p></p><ul><li><p>This allowed him to control and measure their deflection.</p></li></ul><p></p>
10
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What were the key steps in Thomson’s experiment to discover and electron?

1. Set E = 0 and B = 0 and note the position of the spot on screen S due to undeflected beam.

2. Turn on E⃗ and measure the resulting beam deflection.

3. Maintaining E⃗ , now turn on B⃗ and adjust its value until the beam returns to the undeflected position ⇒ with the forces in opposition, they can be made to cancel

<p>1. Set E = 0 and B = 0 and note the position of the spot on screen S due to undeflected beam. </p><p></p><p>2. Turn on E⃗ and measure the resulting beam deflection. </p><p></p><p>3. Maintaining E⃗ , now turn on B⃗ and adjust its value until the beam returns to the undeflected position ⇒ with the forces in opposition, they can be made to cancel</p>