ما الجديد

RC / RL Filter & Time Constant

الإشارة والتوقيت

Cut-off, time constant, rise time and settling to n bits for a one-pole RC or RL filter.

هذه الصفحة غير مترجمة بالكامل بعد. الأجزاء غير المترجمة معروضة بالإنجليزية.

المدخلات

Ω
10 kΩ
F
100 nF
Hz
Hz
1 kHz

النتائج

1 للمراجعة
Cut-off frequency fc

بلا حكم: a corner frequency has no pass or fail. Where it belongs depends on the signals you keep and reject.

−3 dB point

159.2Hz
أظهر خطوات الحساب
  1. Cut-off frequencyf_c = 1 / (2π R C) = 1 / (2π × 10 kΩ × 100 nF) = 159.2 Hz
  2. Time constantτ = R × C = 10 kΩ × 100 nF = 1 ms
  3. Rise time, 10 to 90 %t_r = 2.2 × τ = 2.2 × 1 ms = 2.2 ms
Time constant τ

63.2 % of final value

1ms
Rise time (10–90 %)

tr = 2.2 τ = 0.35/fc

2.2ms
كل النتائج (5)
Capacitance C
100nF
Resistance R
10kΩ
Settling to 12 bits

9.0 time constants

9.01ms
Response at 1 kHz

×0.1572, phase -81.0°

-16.07dB
Noise bandwidth

ENBW = 1.57 · fc for one pole

250Hz
The output impedance reaches 10 kΩ. The next stage needs a much higher input impedance, or the cut-off moves.
low-pass

إلى أي حد نعرف هذا الرقم

مدى دقتها
Exact for ideal parts.

On a real board the capacitor is the main uncertainty: a class 2 ceramic loses much of its value under DC bias and over temperature, which moves the corner.

عملياً يهيمن على عدم اليقين مدخل واحد: Capacitance. ضيّقه يضِق معه الجواب.

يُقاس مقابل

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المسح البارامتري

غيّر مدخلاً واحداً على مدى، وشاهد الإجابة والحكم والهامش عند كل خطوة، جدولاً ومنحنى.Pro

أسوأ الحالات

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Circuit

المبدأ

An RC or RL network is a divider whose ratio changes with frequency. The cut-off fc and the time constant τ are the same fact seen two ways: one sets the attenuation, the other how fast the output settles.

Cut-off frequency
fc=12πRC(RL: fc=R2πL)f_c = \frac{1}{2\pi R C} \qquad \t{(RL: } f_c = \frac{R}{2\pi L}\t{)}
Time constant
τ=RC=12πfc(RL: τ=L/R)\tau = R C = \frac{1}{2\pi f_c} \qquad \t{(RL: } \tau = L/R\t{)}
Low-pass magnitude and phase
∣H∣=11+(f/fc)2φ=−arctan⁡ ⁣(ffc)\left|H\right| = \frac{1}{\sqrt{1+(f/f_c)^{2}}} \qquad \varphi = -\arctan\!\left(\frac{f}{f_c}\right)
High-pass magnitude
∣H∣=f/fc1+(f/fc)2\left|H\right| = \frac{f/f_c}{\sqrt{1+(f/f_c)^{2}}}
Step response
v(t)=Vf(1−e−t/τ)v(t) = V_{f}\left(1 - e^{-t/\tau}\right)
Rise time
tr=2.2 τ=0.35fct_r = 2.2\,\tau = \frac{0.35}{f_c}
10 % to 90 % of the final value.
Settling to n-bit accuracy
tsettle=τln⁡ ⁣(2 n+1)≈0.69 (n+1) τt_{settle} = \tau \ln\!\left(2^{\,n+1}\right) \approx 0.69\,(n+1)\,\tau
12 bits needs about 9 time constants; 16 bits about 12.
Equivalent noise bandwidth
ENBW=π2fc=1.57 fcENBW = \frac{\pi}{2} f_c = 1.57\, f_c
Use this, not fc, to integrate noise through the filter.
  • fcf_c−3 dB cut-off, where |H| = 1/√2 and the phase is 45°
  • τ\tautime constant, 63.2 % of a step in one τ
  • ENBWENBWequivalent noise bandwidth of the single pole
تفاصيل إضافية

Choosing R and C

Only the product RC is fixed. A large R adds thermal noise and is sensitive to bias current and leakage. A small R loads the source. Typical ranges:

  • ADC anti-alias: 100 Ω to 1 kΩ, so the sampling capacitor can recharge.
  • Op-amp feedback and active filters: 1 kΩ to 100 kΩ.
  • Debounce and long timers: 10 kΩ to 1 MΩ, with a film or C0G capacitor. A firmware debounce is often simpler.

Use C0G/NP0 for filters and timing: it is stable and has no DC-bias effect. Use X7R only where a ±15 % shift plus DC-bias loss is acceptable. Never use Y5V in a signal path.

One RC is not enough anti-alias filtering above about 12 bits. A single pole falls at 20 dB/decade, so a signal at 10× fc is only 20 dB down. Oversample, or use a multi-pole active filter.

Cascading

Two identical sections do not make a clean two-pole filter. Buffered, the −3 dB point falls to 0.64 fc. Connected directly, the second section loads the first and it falls to about 0.37 fc. For a true two-pole response, design a Sallen-Key or MFB stage.

Related: ADC Resolution & Noise Budget, for acquisition settling.

إصدار المحرك ⁨1.18.3⁩