Example 1
ΔΦ = 0.02 Wb, Δt = 0.01 s -> |ε| = 2 V.
Type the flux change |ΔΦ| [Wb] and the time Δt [s]. The calculator computes Faraday’s law |ε| = |ΔΦ|/Δt: 0.02 Wb in 0.01 s is 2 V, and in 0.1 s it is 0.2 V. Zero seconds does not divide.
Transformer: U2 = U1 n2/n1. Reactance: XL = 2πfL.
Flux change |ΔΦ| (Wb) and Time Δt (s). The result shows up here.
Faraday in this calculator is the magnitude: |ε| = |ΔΦ|/Δt. At 0.02 Wb in 0.01 s you get 2 V. At 0.02 Wb in 0.1 s you get 0.2 V: ten times longer, ten times smaller EMF. At 1 Wb in 0.5 s you get 2 V again. 1 V = 1 Wb/s.
Two fields: |ΔΦ| in webers, Δt in seconds. The result is in volts. A comma and a period in 0.02 are the same flux. The sign of EMF (Lenz, the minus in ε = −dΦ/dt) does not enter the result: the calculator reports the magnitude.
Δt must be positive. Zero does not divide. Both fields need a number before 2 V can appear. A faster flux change at the same |ΔΦ| gives a larger EMF.
Transformer U2 = U1 n2/n1 is on the neighbouring page and computes a turns ratio, not ΔΦ/Δt. XL = 2πfL is coil reactance at frequency f, not Faraday induction. Lorentz force F = B I l is force on a wire, not a volt.
At 0.2 Wb in 0.02 s, |ε| = 10 V. At 0.005 Wb in 0.02 s it is 0.25 V. At 0.001 Wb in 0.001 s it is 1 V. At 0.08 Wb in 0.04 s it is 2 V again.
Type 0.02 and 0.01, click Calculate, and match 2 V. Then stretch Δt to 0.1 s and see 0.2 V. The current I = Q/t that this EMF can drive is a separate step.
|ε| = |ΔΦ| / Δt
ε = −dΦ/dt (Lenz). Δt > 0, |ΔΦ| > 0. 1 V = 1 Wb/s.
Electromagnetic induction here is |ε| = |ΔΦ|/Δt. 0.02 Wb in 0.01 s is 2 V. In 0.1 s it is 0.2 V. 1 V = 1 Wb/s.
ΔΦ = 0.02 Wb, Δt = 0.01 s -> |ε| = 2 V.
ΔΦ = 0.02 Wb, Δt = 0.1 s -> |ε| = 0.2 V.
ΔΦ = 1 Wb, Δt = 0.5 s -> |ε| = 2 V.
ΔΦ = 0.005 Wb, Δt = 0.02 s -> |ε| = 0.25 V.
ΔΦ = 0.2 Wb, Δt = 0.02 s -> |ε| = 10 V.
ΔΦ = 0.001 Wb, Δt = 0.001 s -> |ε| = 1 V.
ΔΦ = 0.08 Wb, Δt = 0.04 s -> |ε| = 2 V.
ΔΦ = 0.5 Wb, Δt = 0.05 s → |ε| = 10 V.
EMF is 2 V. That is 0.02 / 0.01. At 0.02 Wb and 0.1 s you get 0.2 V: ten times the Δt, one tenth the |ε|.
Flux change |ΔΦ| [Wb], time Δt [s]. Result |ε| [V]. One volt is 1 Wb/s. Type a millisecond as 0.001, not as 1.
The calculator refuses zero seconds. |ε| = |ΔΦ|/Δt at zero time does not exist. Both fields need a number.
No. It computes the magnitude. The Lenz sign, ε = minus dΦ/dt, sits in the formula, not in the result.
Here EMF from flux change over time. There the turns ratio of an ideal transformer, with no ΔΦ field.
Here induction from ΔΦ and Δt. There coil reactance at a known f. Different fields, even though both cards talk about induction.
EMF is 2 V. At 0.2 Wb and 0.02 s you get 10 V. A large flux in a short time drives |ε| up.
Yes. 0.02 and 0,02 are the same |ΔΦ| [Wb]. A comma and a period mean the same value.
EMF is 0.25 V. At 0.001 Wb and 0.001 s you get 1 V. A small flux, a short Δt.
On F = B I l. Here EMF in volts from dΦ/dt, not a force on a wire in teslas.
The formula is the school one. Units follow SI; NIST SP 330 and BIPM define the measures, not your result.
Page updated in 2026.