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Time Constant in AP Physics C: Electricity and Magnetism

In AP Physics C: E&M, the time constant τ is the characteristic time of an exponential circuit change. It equals RC for an RC circuit and L/R for an LR circuit. In one τ, a charging quantity reaches about 63% of its final value, and a decaying quantity falls to about 37%.

This definition is part of Fiveable's AP Physics C: Electricity and Magnetism review, which also has guided practice questions.

Verified for the 2027 AP Physics C: Electricity and Magnetism exam•Last updated October 2026•Fiveable Content Team

What is Time Constant?

The time constant (symbol τ, "tau") tells you how fast a circuit settles into its new steady state after a switch is flipped. Capacitors and inductors don't change instantly. Their charge, voltage, or current approaches the final value along an exponential curve, and τ sets the pace of that curve. A small τ means a fast circuit. A large τ means a sluggish one.

For an RC circuit, τ = RC. For an LR circuit, τ = L/R. Both come out in seconds (Ω·F = s and H/Ω = s, a good units check). The key benchmark is this. After one τ, a growing quantity has reached 1 − e⁻¹ ≈ 63% of its final value, and a decaying quantity has dropped to e⁻¹ ≈ 37% of its starting value. After about 5τ, the circuit is close enough to finished (over 99%) that you can treat it as being at steady state.

Why Time Constant matters in AP® Physics C: E&M

The time constant appears in two CED topics, 11.8 Resistor-Capacitor (RC) Circuits (Unit 11) and 13.5 Circuits with Resistors and Inductors (LR Circuits) (Unit 13). It is the one idea that makes those two topics feel like the same problem with different parts. In both, you write a loop-rule differential equation, solve it, and get an exponential whose rate is set by τ. The AP exam leans on this because it tests calculus-based reasoning (setting up and solving a first-order differential equation) and graph interpretation (reading τ off an exponential curve). It also shows up in lab-design FRQs, where measuring τ is a sneaky way to find an unknown R, C, or L.

How Time Constant connects across the course

Exponential Decay (Units 11, 13)

The time constant is the scale on the exponential decay curve. Every equation you'll write looks like e^(−t/τ), so τ is basically "how many seconds count as one step down the curve." If you know the math of exponential decay, you already know how τ behaves.

Capacitance and Equivalent Capacitance (Units 10, 11)

Because τ = RC, anything that changes C changes the timing. Adding a dielectric, combining capacitors, or finding an equivalent capacitance in Unit 10 directly speeds up or slows down the circuit in Unit 11. A bigger capacitor is a bigger bucket, so it takes longer to fill through the same resistor.

Inductor and LR Circuits (Unit 13)

An inductor resists changes in current, so current in an LR circuit ramps up with τ = L/R instead of jumping. The surprise for most students is that a bigger R makes an LR circuit faster, which is the opposite of an RC circuit. The reason is that a larger R lowers the final current the inductor has to reach.

Energy Stored in a Capacitor or Inductor (Units 10, 13)

Stored energy depends on q² (capacitor) or I² (inductor), so energy decays twice as fast as charge or current. If charge goes as e^(−t/τ), energy goes as e^(−2t/τ). After 2τ, only e⁻⁴ (about 1.8%) of the initial energy is left.

Is Time Constant on the AP® Physics C: E&M exam?

Expect the time constant in both MCQs and FRQs. Common moves include these:

  • Plug and check. Compute τ = RC and compare it to a measurement. For example, a 2.0 μF capacitor with a 3.0 MΩ resistor gives τ = 6.0 s, so reaching 63% of maximum charge at 6.0 s is exactly what theory predicts.
  • Count time constants. Find how many τ it takes to reach a given fraction of the final voltage, using V = V₀(1 − e^(−t/τ)).
  • Write the function. For a discharging capacitor, q(t) = Q₀e^(−t/τ). For charging, q(t) = Q_max(1 − e^(−t/τ)).
  • Energy twist. Since U ∝ q², the energy fraction after time t is e^(−2t/τ).

Released FRQs use τ inside bigger problems. 2021 FRQ Q1 has a battery, resistors, and initially uncharged capacitors with a switch, which is classic RC timing territory. 2018 FRQ Q2 is an experiment built around measuring the dielectric constant of paper in a homemade parallel-plate capacitor. 2024 FRQ Q2 asks you to determine an unknown resistance in a circuit with a battery and an inductor of known value, where τ = L/R (with the right equivalent resistance) is the bridge to R. On lab-style questions, linearizing an exponential (for example, graphing ln of current or voltage against t) gives a slope of −1/τ.

Time Constant vs Half-life

Both describe exponential decay, but they mark different points on the curve. The time constant τ is when a decaying quantity falls to 1/e (about 37%) of its start. The half-life is when it falls to 50%, and it's shorter, t½ = τ ln 2 ≈ 0.69τ. If a problem says "63%" or "37%," think τ. If it says "half," use ln 2.

Key things to remember about Time Constant

  • The time constant is τ = RC for an RC circuit and τ = L/R for an LR circuit, and both have units of seconds.

  • After one time constant, a charging capacitor reaches about 63% of its final charge or voltage, and a discharging capacitor drops to about 37% of its initial value.

  • After roughly five time constants, an RC or LR circuit is effectively at steady state.

  • Increasing R slows down an RC circuit but speeds up an LR circuit, because τ = RC while τ = L/R.

  • Stored energy depends on charge or current squared, so it decays with e^(−2t/τ), twice as fast as the charge or current itself.

  • Graphing the natural log of a decaying voltage or current against time gives a straight line with slope −1/τ, a common lab-FRQ technique.

Frequently asked questions about Time Constant

What is the time constant in AP Physics C E&M?

It's the characteristic time τ that sets how fast an RC or LR circuit changes exponentially. For RC circuits τ = RC, and for LR circuits τ = L/R. In one τ, a growing quantity hits about 63% of its final value.

Is the capacitor fully charged after one time constant?

No. After one τ it's only at about 63% of its final charge. It reaches about 86% at 2τ, 95% at 3τ, and over 99% at 5τ, which is when you can treat it as fully charged.

Does a bigger resistor always make the time constant longer?

No, only in RC circuits. For RC, τ = RC, so a bigger R means a slower circuit. For LR, τ = L/R, so a bigger R actually makes the current settle faster.

How is the time constant different from half-life?

The time constant is when a decaying quantity drops to 1/e (about 37%), while the half-life is when it drops to 50%. They're related by t½ = τ ln 2, so the half-life is about 0.69τ.

What fraction of a capacitor's energy is left after 2τ of discharging?

About 1.8%. Energy is proportional to q², so U = U₀e^(−2t/τ), and at t = 2τ that's e⁻⁴ ≈ 0.018. Charge alone would still be at e⁻² ≈ 13.5%.