Contrast enhanced ultrasound, CEU

Nico A.M. Schellart, Dept. of Med. Physics, AMC

 

Principle

 

CEU is administrating gas-filled microbubbles intravenously to the systemic circulation in echography. Microbubbles in fluid and subjected to an ultrasound field show compressions and rarefactions, so they oscillate strongly and consequently reflect the waves. They are highly echogenetic, due to the large acoustic impedance difference between gas and liquid. There characteristic echo generates the strong and unique echogram in contrast enhanced ultrasound. CEU can be used to image blood perfusion and flow rate in organs.

 

Bubbles in blood are thought to be covered by a surfactant of blood-macromolecules. However, often bubbles with an artificial skin (coating, e.g. phospholipids) are injected. This coating also improves stability and prevents dissolution.

 

The gas core, the contrast agents, is the most important part of the ultrasound contrast signal and determines the echogenicity. They lower the threshold for cavitation (the collapse of the bubble during rarefaction). The reflected signal as well as the signal emitted during cavitation can be used.

Common practiced gases are of N2, or heavy gases like sulfurhexafluoride (F6S), perfuorocarbon and octafluoropropane, which are all inert. Heavy gases are less water-soluble so they leak less to the medium, guarantying long lasting echogenicity. Regardless of the shell or gas core composition, microbubble size is fairly uniform, ranging 1-4 μm in diameter. F6S bubbles have a mean of 2,5 μm and 90%<6 μm. With these sizes, they flow easily through the microcirculation.

Selection of shell material determines how easily the microbubble is taken up and how long the bubbles survive.

 

Targeting ligands that bind to receptors characteristic of intravascular diseases can be conjugated to themicrobubble skin, enabling the microbubble complex to accumulate selectively in areas of interest. However, the targeted technique has not yet been approved for clinical use; it is currently under preclinical research and development.

Genetic drugs can incorporated into ultrasound contrast agents. Genebearing microbubbles can be injected IV and ultrasound energy applied to the target region. As the microbubbles enter the region of insonation, the microbubbles cavitate, locally releasing DNA. Cavitation also likely causes a local shockwave that improves cellular uptake of DNA. By manipulating ultrasound energy, cavitation and so delivery can be visualized in the vessels with bubbles. Imaging can be performed before, just after IV and during cavitation, each with a different energy, to control the process of delivery.

Applications

Untargeted CEU is currently applied in echocardiography. Microbubbles can enhance the contrast at the interface between the tissue and blood. When used in conjunction with Doppler (see Doppler principle) Ultrasound, microbubbles can measure myocardial flow rate to diagnose valve problems. The relative intensity of the microbubble echoes can also provide a quantitative estimate on blood volume.

In vascular medicine, bubbles visualize perfusion. Therefore this technique is crucial for tracking down a  and so stenosis.

 

Targeted CEU is being developed for a variety of medical applications. Microbubbles targeted with ligands are injected systemically in a small bolus. The ligands bind to certain molecular markers that are expressed by the area of imaging interest Microbubbles theoretically travel through the circulatory system, eventually finding their respective targets and binding specifically. Ultrasound waves can then be directed on the area of interest.

Specific applications are to visualize for instance inflammatory organs (Crohn’s disease, arteriosclerosis, heart attacks).

Microbubbles-targeted ligands can bind receptors like VEGF to depress angiogenesis in areas of cancer. Detection of bound targeted microbubbles may show the area of expression. This can be indicative of a certain disease state, or may identify particular cells in the area of interest.

Drugs can be incorporated into the microbubble’s lipid shell. The microbubble’s large size relative to other drug delivery vehicles like liposomes may allow a greater amount of drug to be delivered per vehicle. By targeted the drug-loaded microbubble with ligands that bind to a specific cell type, microbubble will not only deliver the drug specifically, but can also provide verification that the drug is delivered if the area is imaged using ultrasound. Local drug delivery is used for angiogenesis, vascular remodeling andr tumor destruction.

The force associated with the bursting may temporarily permeabilize surrounding tissues and allow the DNA to more easily enter the cells. This can further be facilitated by coating materials of the shell, e.g. liposomes, positively charged polymers, and viruses (as they do already for millions of years for delivering genetic materials into living cells).

 

More info

 

Gas bubbles in a liquid are characterized by a resonance frequency f, which is directly related to their diameter R0. f can by approximated (liquid surface tension not included; S. De, 1987) by:

   (1)

with γ the specific heat ratio of the gas (=1.40 for N2; see Gas laws), ρl the liquid density (=1050 kg/m3 for blood) and P0 the ambient pressure (here 114.7 kPa).  With R0=2.5 μm, f is about 1.36 MHz. With  R0>100 μm (1) is accurate but with R0≤10 μm f is about 3.5% too small. Implying the surface tension of blood (=0.058 N/m) would increase f with 7.7%, but bubbles of this size will be surrounded by a surfactant skin, which counteracts the effect of the surface tension (see More info of Surface tension). In pure water, bubbles have an extremely sharp resonance peak (quality Q about 70) but in blood and with the skin surfactant, this is much lower due to the skin-shear and skin-stiffness. With the heavy multiatomic gases f is smaller since γ is smaller (for F6S γ =1.10) and ρl considerably larger.

 

 

Fig. 1 Different MIs produce different reflected spectra.

 

Micro-bubbles oscillate (expand and contract) in the ultrasound field. The pattern and nature of their oscillation, and thus the nature of the backscatter signal, differs, depending on the transmitted acoustic power. The power of the ultrasound field is expressed as the mechanical index (MI; see Ultrasound). With very low MI (< 0.1), micro bubbles demonstrate linear oscillation (reflected frequency equals impeding frequency). Low MIs (0.1 – 0.6), generates nonlinear oscillation of the micro bubble whereby expansion is greater than contraction. In addition to the usual backscatter of the fundamental frequency, the bubbles also produce backscatter of harmonics (see Signal analysis and Fourier). When exposed to high MI (> 0.6, i.e. the MI used for standard imaging) the bubbles oscillate wildly and burst. Upon destruction, micro-bubbles produce a brief, high amplitude signal, with good resolution, which is rich in harmonic signals, containing backscatter at the second third and fourth harmonics etc (Fig. 1).

The most important limitation of this technique is motion artifact from tissue, because tissue motion will be expressed like bubble destruction, potentially showing perfusion when none is present (a false negative). If Doppler frequency is increased, pulse separation is reduced, so tissue movement between pulses can be minimized. However, if the pulses are too close, not all the gas within the bubble will have dissipated before arrival of the next pulse, so the difference between pulses is reduced, possibly leading to false positive perfusion defects. Air-filled micro-bubbles are optimal for this technique because of rapid dissipation of the gas, allowing closely spaced pulses.

There are several high MI techniques, some developed for the moving myocard.

 

Triggered harmonic imaging

Intermittent high power imaging can improve imaging, with the best opacification obtained using intermittent harmonic imaging. During intermittent high power imaging, high energy ultrasound is transmitted at specified intermittent intervals, triggered to the ECG (e.g. 1 of 4  cardiac cycles). The time between destructive pulses allows the micro-bubbles to replenish the myocardium. With each destructive pulse, high amplitude backscatter rich in harmonics is returned to the transducer, enabling static images of myocardial perfusion.

 

 

Fig. 2 From top to bottom: Base imaging, no bubbles; contrast, bubbles; subtracted, echo’s subtracted; gray-scale, color coded.

 

Pulse Inversion Doppler

Another grey scale high MI technique is pulse-inversion imaging whereby two synchronized beams of pulses impinging onto the myocardium. The second pulse sent is a mirror image of the first (i.e. 180° phase shift). The scanner processes the echo’s of two types of pulses by adding them together. When the bubbles generate a linear echo, the addition of one pulse to the other should cancel out to zero and no signal is generated. However, micro-bubbles produce non-linear echo signals at high MI and the summation of returning pulses will not equal zero.

Using this technique, processing can theoretically be limited only to signals generated by bubbles and not by other objects.  However, tissue motion artefacts are a major limitation, as movement of tissue also creates non-linear signals.

 

More specific applications can be found in ref. 5.

 

Physical advantages of CEU  

Ø       Ultrasonic molecular imaging is safer than molecular imaging modalities such as radionuclide imaging.

Ø       Since microbubbles can generate such strong signals, a lower intravenous dosage is possible; micrograms compared to milligrams for other molecular imaging modalities such as MRI contrast agents.

Physical disadvantages of CEU   

Ø       Ultrasound produces more heat as f increases, so f must be carefully monitored.

Ø       Equipment settings are subjected to safety indexes (see Ultrasound). Increasing ultrasound energy increases image quality, but microbubbles can be destructed, resulting in microvasculature ruptures and hemolysis.

Ø       Low targeted microbubble adhesion efficiency, which means a small fraction of injected microbubbles bind to the area of interest.

 

Literature

1 De S. On the oscillations of bubbles in body fluids. J Acoust Soc. Amer, 1987, 81, 56-567.

2 Postma, M., Bouakaz A., Versluis M. and de Jong, N. IEEE T Ultrason Ferr, 2005, 52, in press.

3 http://en.wikipedia.org/wiki/Contrast_enhanced_ultrasound

4 http://e-collection.ethbib.ethz.ch/ecol-pool/diss/fulltext/eth15572.pdf

5 http://www.cardiovascularultrasound.com/content/2/1/15