Accelerating a charged particle through a set voltage is a direct way to give it a known amount of kinetic energy. On paper, the math is straightforward, but expressing that energy in joules quickly lands you with extremely small numbers — not practical when working at the atomic or subatomic level. This calculator gives you a fast conversion to electron volts (eV), keV, MeV, or joules based on voltage, charge state, and particle count. These conversions show up everywhere: semiconductor ion injection, X-ray generators, electron microscopes, and for anyone dealing with particle beams. To keep things useful, this page lays out conversion formulas, a worked TEM example, some notes on relativity, and a detailed FAQ.
What is an Electron Volt?
An electron volt (eV) is simply the energy an electron gets from moving through a 1 volt difference. It's the go-to unit for atomic and particle physics because you get practical numbers that don't hide behind a pile of zeroes.
Simple Explanation
Voltage, in this application, is like a ramp for charged particles: boost the voltage, and your charged particle gets a proportional jump in energy — no more, no less. When you run one electron across 1 volt, that's 1 electron volt. If your particle carries more charge, you multiply the effect — a two-charge ion gets twice the energy at the same voltage.
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Table of Contents
How to Use This Calculator
- Select your calculation mode from the dropdown — choose from Volts to eV, eV to Volts, keV, MeV, multi-charge ion energy, or photon wavelength.
- Enter your voltage (V) or energy in eV, depending on the selected mode. For multi-charge ion mode, also enter the charge state (z) and number of particles.
- If using multi-charge mode, confirm the charge state and particle count fields are filled with valid positive values.
- Click Calculate to see your result.
Simple Example
Mode: Volts to Electron Volts (eV)
Input: Voltage = 5 V
Result: Energy = 5 eV = 0.005 keV = 0.000005 MeV = 8.011 × 10⁻¹⁹ J
A single electron accelerated through 5 V gains exactly 5 eV of kinetic energy.
Visual Diagram
Volts To Electron Volts Interactive Calculator
This calculator is intended for education, concept evaluation, and preliminary design. Results are based on the equations and assumptions described on this page, but cannot account for every real-world load case, tolerance, material property, environmental condition, installation detail, safety factor, code, or regulatory requirement. Verify all inputs, assumptions, units, and results independently before selecting components or using the result in a real application. Safety-critical, structural, medical, lifting, transportation, or regulated applications must be reviewed by a qualified engineer.
Conversion Equations
To get energy in electron volts from voltage, use the simple formulas below.
Basic Conversion (Single Electron)
EeV = V
EJ = V × e
where e = 1.602176634 × 10-19 C (elementary charge)
Multi-Charge Ion Energy
EeV = V × z
where z is the charge state (number of elementary charges)
Photon Energy to Wavelength
λ = hc / EJ
λ = hc / (V × e)
where h = 6.62607015 × 10-34 J·s (Planck constant), c = 299,792,458 m/s (speed of light)
SI Unit Prefixes
1 keV = 103 eV
1 MeV = 106 eV
1 GeV = 109 eV
Theory & Practical Applications
The electron volt is just the energy a single electron picks up across 1 volt. This makes it easy to bridge standard bench voltages to the much smaller energy scales at the atomic level. When you need to keep the math straightforward (and the numbers accessible) in particle and atomic physics, the eV is the right tool for the job.
Physical Foundation and Non-Obvious Implications
The EeV = V relationship really just leans on the work-energy theorem for tiny objects. This says if you push a charge q through a potential ΔV, you get ΔE = qΔV. Set q to an electron's charge and the math is as simple as counting the volts — but that only works if you're dealing with one electron. If you have an ion (like He2+), you’re getting double the energy from the same voltage, and this adds up fast in instruments like mass spectrometers. There, you can't ignore that charge state, because it's not just tuning energy — it shifts everything from velocity to how you read the timing.
Relativity doesn't matter until you crank energies high enough. Below a few keV for electrons, the old kinetic energy formula does alright. But if you accelerate particles into the MeV range, “½mv²” gives answers that aren’t physically possible (like speeds over the speed of light). You need to use E = (γ - 1)mc² with γ = 1 / sqrt(1 - v²/c²). As an example, a 10 MeV electron is nowhere near what a classical calculation would suggest for its speed. For real-world electron beams used in semiconductor writing or therapy systems, ignoring relativity at high voltages gives the wrong velocities and lens requirements.
Industrial Applications Across Energy Scales
Semiconductor Manufacturing (1-100 keV): Ion implant tools set the penetration depth into silicon almost entirely by the acceleration voltage. If you run 20 mA of boron ions at 50 keV, that’s 1 × 1015 ions per second, each one carrying 50 keV. All that energy comes out as heat — about 1000 W — so if you don’t cool the wafer, you’ll damage it. The depth an ion reaches in silicon scales roughly as E2/3 over the atomic density of the wafer, so you have to get both your voltage and doping rate right for precision doping.
X-Ray Tube Technology (20-150 kV): In basic X-ray tubes, the acceleration voltage tells you the maximum photon energy you’ll produce. Medical chest X-ray systems at 120 kV produce photons up to 120 keV. Lower voltages don’t penetrate as deeply or give the same image contrast. The X-ray intensity comes from tube current, but the penetration (and image type) comes from voltage. If you’re analyzing materials using the emission lines (like tungsten’s Kα at 59.3 keV), you’re also tuning voltage for those peaks.
Particle Physics Research (GeV-TeV): In big accelerators like the LHC, you’re working with voltages and energies so high the rest mass barely matters — everything is close to the speed of light. The magnetic fields required to bend those beams get dictated by the particle momentum, not just their energy. For protons at 6.5 TeV, the magnetic rigidity is huge, and the collider only works because of high-field superconducting magnets running near absolute zero.
Worked Example: Multi-Stage Electron Microscope Acceleration
Scenario: A TEM accelerates electrons in three steps (5 kV, 100 kV, 300 kV). What's the beam energy, electron velocity, and resulting minimum resolvable size?
Given:
- Stage 1 voltage: V₁ = 5 kV
- Stage 2 voltage: V₂ = 100 kV
- Stage 3 voltage: V₃ = 300 kV
- Electron rest mass: me = 9.10938 × 10-31 kg
- Elementary charge: e = 1.602176634 × 10-19 C
- Planck constant: h = 6.62607015 × 10-34 J·s
- Speed of light: c = 2.99792458 × 108 m/s
Solution:
Step 1: Calculate total electron energy
Total accelerating voltage: Vtotal = 5 + 100 + 300 = 405 kV
Kinetic energy: Ek = 405 keV = 405,000 eV
In joules: Ek = 405,000 × 1.602176634 × 10-19 = 6.4888 × 10-14 J
Step 2: Calculate relativistic parameters
Electron rest mass energy: E₀ = mec² = 0.511 MeV = 511,000 eV
Since Ek = (γ - 1)E₀:
γ - 1 = Ek/E₀ = 405,000 / 511,000 = 0.7925
γ = 1.7925
Step 3: Calculate electron velocity
From γ = 1/√(1 - v²/c²), we solve for v:
v²/c² = 1 - 1/γ² = 1 - 1/(1.7925)² = 1 - 0.3112 = 0.6888
v = 0.8299c = 2.488 × 108 m/s
Step 4: Calculate de Broglie wavelength
Relativistic momentum: p = γmev = 1.7925 × (9.10938 × 10-31) × (2.488 × 108)
p = 4.063 × 10-22 kg·m/s
de Broglie wavelength: λ = h/p = (6.62607015 × 10-34) / (4.063 × 10-22)
λ = 1.631 × 10-12 m = 1.631 pm
Step 5: Estimate resolution limit
For diffraction-limited resolution with objective lens half-angle α ≈ 10 mrad (typical for high-resolution TEM):
Rayleigh criterion: dmin = 0.61λ/sin(α) ≈ 0.61λ/α (small angle approximation)
dmin = 0.61 × (1.631 × 10-12) / (0.010) = 9.95 × 10-11 m = 0.995 Å
Result Interpretation: With 405 kV, electron wavelength dips below 2 pm, making true atomic-resolution imaging possible. Relativistic effects are significant (gamma factor nearly 1.8), and lens designs must account for this mass increase. The roughly 1 Å resolution fits typical distances between atoms in solid materials, which is why modern TEMs can directly “see” individual atomic columns.
For detailed unit conversion workflows, visit our comprehensive engineering calculator library.
Energy Scale Context and Practical Boundaries
Just knowing the scale of eV values helps put quantum energies into perspective:
- Thermal energy at room temperature: kT ≈ 26 meV (chemistry, vibrational modes)
- Visible light photons: 1.7-3.1 eV (photos, LEDs, solar cells)
- Ionization energies: 5-25 eV (freeing valence electrons, starting plasmas)
- Medical X-rays: 20-150 keV (diagnostic images, bone contrast)
- Gamma ray therapy: 1-20 MeV (deep tissue dose)
- Cosmic ray primaries: GeV-EeV (atmospheric showers)
If you’re working below 1 keV with electrons, classical calculations stay pretty close (gamma ≈ 1.002). For protons, you stay non-relativistic up to a few MeV, thanks to much higher rest mass energy.
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About the Author
Robbie Dickson — Chief Engineer & Founder, FIRGELLI Automations
Robbie Dickson brings over two decades of engineering expertise to FIRGELLI Automations. With a distinguished career at Rolls-Royce, BMW, and Ford, he has deep expertise in mechanical systems, actuator technology, and precision engineering.
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