SLVSHH0 June 2026 TPS61290
PRODMIX
The TPS61290x uses a hysteretic control scheme, and TPS61290x maintains a constant inductor ripple current in the range of 3.0A. Therefore, the frequency is not fixed and determined by the operation condition. The frequency is approximately 2MHz, when the input is 2.7V, output is 3.4V, inductor is 100nH.
In auto PFM operation, the minimum switching frequency is not limited, the switching frequency is approximately 20Hz (or even lower) with open load.
In forced PWM operation, minimum switching frequency is limited to approximately 375kHz. With this unique feature, the TPS61290x avoids the low frequency switching and prevents the application against the low frequency noise sensitive range.
Switching regulators are particularly troublesome in applications where electromagnetic interference (EMI) is a concern. Switching regulators operate on a cycle-by-cycle basis to transfer power to an output. In most cases, the frequency of operation is either fixed or regulated, based on the output load. This method of conversion creates large components of noise at the frequency of operation (fundamental) and multiples of the operating frequency (harmonics).
The TPS61290x provides a spread spectrum feature. The goal is to spread out the emitted RF energy over a larger frequency range so that the resulting EMI is similar to white noise. The result is a spectrum that is continuous and lower in peak amplitude, making complying with electromagnetic interference (EMI) standards and with the power supply ripple requirements in cellular and non-cellular wireless applications easier. Radio receivers are typically susceptible to narrowband noise that is focused on specific frequencies.
The spread spectrum architecture varies the switching frequency by ca. ±8% of the nominal switching frequency thereby significantly reducing the peak radiated and conducting noise on both the input and output supplies. The frequency dithering scheme is modulated with a triangle profile and a modulation frequency fm.
The above figures show that after modulation the sideband harmonic is attenuated compared to the non-modulated harmonic, and the harmonic energy is spread into a certain frequency band. The higher the modulation index (mf) the larger the attenuation.
where
The maximum switching frequency fc is limited by the process and finally the parameter modulation ratio (δ), together with fm, which is the side-band harmonics bandwidth around the carrier frequency fc. The bandwidth of a frequency modulated waveform is approximately given by the Carson’s rule and can be summarized as:
fm < RBW: The receiver is not able to distinguish individual side-band harmonics, so, several harmonics are added in the input filter and the measured value is higher than expected in theoretical calculations.
fm > RBW: The receiver is able to properly measure each individual side-band harmonic separately, so the measurements match with the theoretical calculations.