How to Use the Calculator?
To use the calculator, choose your configuration (RC, RL, or LC) and enter any two input values. The calculator will then compute the remaining value.
What is a High-Pass Filter?
A high-pass filter is an electronic filter that passes signals with a frequency higher than a certain frequency, called cut-off frequency, and attenuates signals with frequencies lower than the cutoff frequency. It is sometimes called a low-cut filter or bass-cut filter in the context of audio engineering.
A high-pass filter can be constructed using resistors, inductors, and capacitors. When designing a filter, it’s crucial to understand how each element influences the signal. The resistor element is typically frequency independent. The inductor’s impedance increases as frequency increases, whereas the capacitor’s impedance decreases.
Taking into account these distinct characteristics, various filter configurations, such as the RC Filter, RL Filter, and LC Filter, have been designed.
RC filters use resistors and capacitors, RL filters use resistors and inductors, and LC filters use capacitors and inductors. Each type of filter has its own advantages and disadvantages, depending on the application and the desired characteristics.
RC Filter
A simple first-order RC high-pass filter consists of only one resistor and one capacitor connected in series, with the output taken across the resistor.

In this configuration, the capacitor’s reactance is very high at low frequencies so the capacitor acts as an open circuit and blocks any input signals until the cut-off frequency point (Fc) is reached. Beyond this point, the capacitor’s reactance decreases significantly, causing the capacitor to behave more like a short circuit and allowing the input signal to pass directly to the output.
In an RC filter, the resistor and capacitor together create a time constant that defines the cutoff frequency. This can be calculated using the formula:
$$F_c = \frac{1}{2\pi RC}$$
Where,
$F_c$ is the cutoff frequency in hertz,
$R$ is the resistance in ohms,
and $C$ is the capacitance in farads.
A first-order RC filter has a slope of +20 dB/decade, which means that for every factor-of-ten increase in frequency, the gain increases by 20 dB until the frequency reaches the cut-off point.
Response curve of an RC filter can be illustrated as:

A higher-order RC filter can be obtained by cascading multiple first-order RC filters. A higher-order filter has a steeper slope and a sharper transition from the passband to the stopband, but it also introduces more phase distortion and complexity.
RL Filter
A simple first-order RL high-pass filter consists of only one resistor and one inductor connected in series, with the output taken across the inductor.

In this configuration, the inductor’s impedance increases as the frequency increases, while the resistor allows all frequencies to pass through. This means that the inductor acts as an open circuit for high-frequency signals and a short circuit for low-frequency signals, thus passing the high frequencies.
The cutoff frequency for an RL circuit is not as well defined as for an RC circuit because the response does not have a simple mathematical expression. However, a rough estimate of the cutoff frequency can be obtained using the formula:
$$F_c = \frac{R}{2\pi L}$$
Where,
$F_c$ is the cutoff frequency in hertz,
$R$ is the resistance in ohms,
and $L$ is the inductance in henrys.
A first-order RL filter has a slope of +20 dB/decade, which means that for every factor-of-ten increase in frequency, the gain increases by 20 dB until the frequency reaches the cut-off point.
LC Filter
A simple first-order LC high-pass filter consists of only one inductor and one capacitor connected in series, with the output taken across the inductor.

The cutoff frequency of this filter is given by the formula:
$$F_c = \frac{1}{2\pi \sqrt{LC}}$$
Where,
$F_c$ is the cutoff frequency in Hertz,
$L$ is the inductance in henrys,
and $C$ is the capacitance in farads.
A first-order LC filter has a slope of +40 dB/decade, which means that for every factor-of-ten increase in frequency, the gain increases by 40 dB until the frequency reaches the cut-off point.
