Dynamically Induced EMF Calculator
e = B l v sin θ • Conductor cutting a magnetic field • Fleming’s right-hand rule
When a conductor moves in a stationary magnetic field and cuts the flux,
an emf is induced in it — a dynamically induced emf. Its value is
e = B l v sin θ, where θ is the angle between the direction of motion and the field.
Only the part of the velocity perpendicular to the field, v sin θ, cuts flux.
📘 How to Use (tap to hide / show)
- 1Choose what to find: emf e, flux density B, length l, velocity v or angle θ.
- 2Enter the other values and pick their units (cm, km/h, mT…) — the calculator converts them to SI units.
- 3Set the angle θ between v and B with the box or the slider. The diagram shows it immediately.
- 4Click ⚡ Calculate to get the answer, the step-by-step working and the emf direction (⊗ / ⊙).
1
What Do You Want to Find?
2
Enter the Known Values
Field direction:
3
Diagram – Conductor Moving in the Field
Magnetic field B
Velocity v
v sin θ (cuts flux)
v cos θ (no emf)
⊗ current into page ⊙ out of page
✓ Result
Step-by-step Solution
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Fleming’s Right-Hand Rule and Special Cases
Fleming’s Right-Hand Rule (generator rule)
Stretch the thumb, first finger and second finger of the right hand mutually at right angles:
- Thumb → direction of Motion of the conductor
- First finger → direction of Field (N to S)
- Second finger → direction of induced Current / emf
Special cases of e = B l v sin θ
| Angle θ | Motion | Induced emf |
|---|---|---|
| 0° or 180° | Parallel to the field | e = 0 (no flux cut) |
| 90° | Perpendicular to the field | e = B l v (maximum) |
| Any other θ | At an angle | e = B l v sin θ |
Statically vs dynamically induced: in a dynamically induced emf the conductor moves (generator); in a statically induced emf nothing moves and the flux itself changes (self-induced, mutually induced — transformer).
Note: B in tesla (1 T = 1 Wb/m²), l = active length of the conductor inside the field in metres,
v in m/s. θ is measured from the direction of B to the direction of v, anticlockwise, from 0° to 360°
when finding e (180°–360° means the conductor moves the other way, so the emf reverses).
When finding B, l, v or θ, enter the size of the emf and an angle between 0° and 180°.
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