(TI) The definition of the thermal index is the ratio of the total acoustic power to that required raising a maximum temperature increase of 1 °C under defined assumptions. A thermal index of 1 indicates the acoustic power achieving a temperature increase of 1 °C. A thermal index of 2 has the doubled power but would not necessarily indicate a peak temperature rise of 2 °C. The temperature rise is dependent on tissue type and is particularly dependent on the presence of bone.
Classifications of thermal indices:
For fetal ultrasound, the highest temperature increase would be expected occurring at bone. Therefore, TIB gives the worst-case conditions. If the ultrasound system can exceed an index of 1, the mechanical index and thermal index must be displayed. The displayed indices are based on the manufacturer's data.

See also Cranial Bone Thermal Index, Bone Thermal Index, Soft Tissue Thermal Index.

The backscatter energy is the portion of the incident acoustic power scattered back toward the transducer.

Ultrasound waves are reflected when there is a change in acoustic impedance. The larger the change, the more ultrasound is reflected. Microbubbles have an enormous difference in acoustic impedance as compared to surrounding fluid due to the large differences in density, elasticity and compressibility.
At low acoustic power (mechanical index less than 0.1), the mechanism of ultrasound reflection is that of Rayleigh scattering and the microbubbles may be regarded as point scatterers. The scattering strength of a point scatterer is proportional to the sixth power of the particle radius and to the fourth power of the ultrasound frequency;; the echogenicity of such contrast agent is therefore highly dependent upon particle size and transmit frequency. The backscattered intensity of a group of point scatterers is furthermore directly proportional to the total number of scatterers in the insonified volume. The concentration of the contrast medium is of importance.

See also Backscatter Energy, Cross-section Scattering.

Ultrasound at the microbubble resonance frequency can cause bubble rupture at high acoustic power (mechanical index (MI) greater than 0.5). The result is a transient high-amplitude, broadband signal containing all frequencies, not only the harmonics. It will create a strong signal in B-mode or a short-lasting multicolored, mosaic-like effect in color Doppler sonography.
Several terms for this typical signal have been used, e.g. induced or stimulated acoustic emission, loss of correlation imaging and sono-scintigraphy.

The dead or ring down zone is the distance from the front face of the transducer to the first echo that is identifiable. The signals from this region are unsuitable. The dead zone is the result of transducer ringing and reverberations from the interface between the transducer and the scanned object. Impedance matching between the transducer and the receiver is important to avoid electrical ringing.
With an increase of the frequency, the pulse length and the depth of the dead zone decrease, if all other parameters remain constant. The acoustic power also affects the depth of the dead zone.