📺Charged Particle Deflection - CRT, Electric Field Deflection, AC Plates
This tool covers the classic exam model of a charged particle accelerated through U₁ and then sent between deflecting plates. The canvas draws the path, the back-extended exit line and the spot on the screen, and every formula is shown with your numbers substituted. Extra tabs show different ions sharing one path, a CRT oscilloscope sweep, an electron beam between alternating plates and straight-line acceleration, with randomized practice at the end.
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How to use Charged Particle Acceleration & Deflection
- 1Pick a particle (electron, proton, deuteron, alpha) and set U₁, U₂, plate length L, gap d and screen distance D
- 2Press Play to watch it accelerate, bend and hit the screen; read v₀, offset y, tanθ, screen offset Y and the critical voltage
- 3Switch to the CRT or AC tab and change the sweep, the signal, the period and the entry time to see the screen picture and exit offsets
- 4Try the random problems on the Practice tab and check the worked solution
FAQ
- Why does the offset y = U₂L²/(4U₁d) not depend on charge or mass?
- Acceleration gives qU₁ = ½mv₀², so mv₀² = 2qU₁. Between the plates y = ½(qU₂/md)(L/v₀)² = qU₂L²/(2mdv₀²). Substituting mv₀² cancels both q and m, leaving y = U₂L²/(4U₁d). Ions of the same sign accelerated from rest by the same voltage and sent through the same plates therefore follow identical paths; they just take different times.
- Why does the exit velocity line pass through the centre of the plates?
- At the exit the offset is y = ½at², the vertical velocity is v_y = at and the horizontal distance is L = v₀t. Extending the exit velocity backwards covers a horizontal distance y/tanθ = (½at²)/(at/v₀) = v₀t/2 = L/2. So the particle seems to come straight from the plate centre, and the screen offset is simply Y = (L/2 + D)tanθ.
- How do I know whether the particle hits a plate?
- For entry along the centre line it hits when the computed offset exceeds d/2. Setting y = d/2 gives the critical voltage U₂ = 2U₁d²/L². With a larger U₂ the particle lands at x = d√(2U₁/U₂) from the entrance. The tool lists the critical voltage and marks the landing point on the canvas.
- Why does an oscilloscope put a sawtooth on the X plates?
- A sawtooth rises linearly, moving the spot across the screen at a steady speed, which turns the horizontal axis into a time axis; then it snaps back and the next sweep starts. The signal on the Y plates moves the spot up and down at the same time, so the screen draws the signal against time. When the sweep period is a whole number of signal periods every sweep lands on the same curve and the picture is stable.
- When do particles leave alternating plates parallel to them?
- When the transit time is a whole number of voltage periods. With a square wave each period pushes the particle one way for half a period and brakes it for the other half, so the vertical velocity returns to zero and every particle leaves parallel to the plates. The one entering at t = 0 is displaced most, y = aT²/4 per period; drag the entry-time slider to see the offset change.
Features
- Full accelerate-then-deflect model: parabolic path, exit line through the plate centre, plate hits and critical voltage
- Proton, deuteron and alpha fired together: same path, different speeds, animated at the true speed ratio
- CRT oscilloscope: sawtooth sweep with sine, square or triangle signals, phosphor afterglow, rolling traces and Lissajous figures
- Alternating plates: continuous beam animation, u–t, v_y–t and y–t graphs, fraction hitting the plates
- Straight-line acceleration and braking: gets through or turns back, stopping depth and v–t graph
- Seven kinds of random problems marked with 2% tolerance and step-by-step solutions
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