Solenoid Electromagnet Force Calculator
Calculate electromagnetic pull force, flux density, and ampere-turns for solenoid coils and electromagnet design.
Electromagnet Design Formulas
Ampere-Turns: At = N × I
Pole Area: A = π × (d/2)²
Pull Force (approx): F = (B² × A) / (2μ₀)
Flux Density (empirical): B ≈ (μ₀ × At) / (length + gap)
Power: P = V × I (coil dissipation)
Solenoid Application Examples
| Application | Typical Force | Voltage/Current | Duty Cycle |
|---|---|---|---|
| Relay Coil | 0.1–1 N | 5–24V, 50–200mA | Intermittent |
| Door Lock Solenoid | 10–50 N | 12–24V, 1–2A | Pulse |
| Solenoid Valve (Gas/Fluid) | 20–100 N | 24V, 0.5–1.5A | Continuous |
| Linear Actuator | 50–200 N | 12–48V, 2–5A | Intermittent |
Frequently Asked Questions
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A solenoid is a coil of wire wound in a tight, helical pattern. When current flows through it, the coil generates a magnetic field. An iron core inserted into the coil amplifies the field, creating a strong pull force. Solenoids are used in relays, door locks, valves, and actuators.
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Exact calculation is complex (requires finite element analysis), but approximations work for design: F ≈ (B² × A) / (2μ₀), where B is flux density (tesla), A is pole area (m²), and μ₀ is permeability. Alternatively, empirical models: F ∝ N²I² (proportional to square of turns and current).
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(1) More turns (N) → more ampere-turns → stronger field. (2) Higher current (I) → stronger magnetization. (3) Shorter air gap → stronger pull (force ∝ 1/gap²). (4) Larger iron core cross-section → more flux capacity. (5) Iron material (soft iron best; steel acceptable).
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Ampere-turns = Coil turns × Current (N × I). Higher ampere-turns = stronger magnetic field. Typical design: 1000–5000 At for small relays, 10,000+ At for powerful solenoids. At is independent of coil geometry—you can achieve same At with many turns at low current or fewer turns at high current.
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Flux density (B, in tesla) measures magnetic field strength. Typical values: air ~0 T (reference), iron core 0.5–1.5 T, saturated iron ~2 T. Higher B = stronger pull force. Magnetic saturation limits B (iron saturates around 2 T; no benefit from more current beyond saturation).
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Force drops dramatically with air gap: F ∝ 1/x², where x is gap. Doubling the gap reduces force to 1/4. This is why solenoid valves have tight tolerances and why electromagnets are most powerful when armature touches pole face.
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Saturation occurs when the iron core can no longer absorb more magnetic flux (B ≈ 2 T for iron). Beyond saturation, adding more current does not increase force—it just creates heat. Good designs operate near (but not into) saturation to maximize force while minimizing coil loss.
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Wire size depends on desired current and power budget. Higher current → thicker wire. Typical: solenoid coils run 1–10 A. Use AWG wire charts: smaller AWG = thicker. Example: 10 A, 10 m coil length → ~14 AWG (1.6 mm). Account for voltage drop and insulation temperature rating.
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A relay is a solenoid with electrical contacts. Current through the coil pulls an armature, which physically moves contacts to switch another circuit. Solenoids just provide mechanical force; relays add electrical switching capability.
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Most solenoids are designed for intermittent duty (short pulses). Continuous operation causes excessive heating. If continuous operation is required, use a "continuous-duty" solenoid with better cooling and lower resistance, or use a latching solenoid that requires only brief pulses.
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Non-latching: coil must be energized continuously to maintain force. Latching: a brief pulse magnetizes a permanent magnet; force is held without current. Latching solenoids save power but are more complex. Used in door locks, automotive, and battery-powered devices.
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Small relays: 5–24 VDC, 10–100 mA. Medium solenoids: 12–24 VDC, 500 mA–2 A. Large solenoids: 24–48 VDC, 2–10 A. Always verify datasheet; over-voltage increases current and force but risks coil burnout. Under-voltage reduces force below usable minimum.