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. Author manuscript; available in PMC: 2015 Mar 6.
Published in final edited form as: J Nucl Med. 2010 Jul 21;51(8):1167–1170. doi: 10.2967/jnumed.109.068981

Tumor pH and its measurement

Xiaomeng Zhang 1, Yuxiang Lin 2, Robert J Gillies 3
PMCID: PMC4351768  NIHMSID: NIHMS570206  PMID: 20660380

Abstract

Studies over the last few decades have demonstrated that intracellular pH (pHi) of solid tumors is maintained within a pH range of 7.0-7.2, while the extracellular pH (pHe) is acidic. A low pHe may be an important factor inducing more aggressive cancer phenotypes. Research into causes and consequences of this acid pH of tumors are highly dependent on accurate, precise and reproducible measurements, and these have undergone great changes since in the last decade. This review focuses on most recent advances of in vivo tumor pH measurement by pH-sensitive Positron emission tomography (PET) radiotracers, magnetic resonance spectroscopy (MRS), magnetic resonance imaging (MRI) and optical imaging.

Keywords: pH, Tumor, PET, MRS, MRI, Optics

Cause and consequences of tumor acidity

The physiological microenvironment of solid tumors is normally characterized by poor perfusion and high metabolic rates. As a consequence, many regions within tumors are transiently or chronically hypoxic and acidic. Acidity is likely related to glucose consumption rates. High fluorodeoxyglucose (FDG) consumption has been consistently shown to be a poor prognostic indicator in human cancers. The pH of cells and tissues is the result of the balance between the metabolic processes, proton transport and buffering. Catabolism of sugars or fats results in a net production of acid, whether through fermentation or respiration (1) (FIGURE 1). The pyruvate made by glycolysis or amino acids can either enter the tricarboxylic acid (TCA) cycle through pyruvate dehydrogenase or be reduced to lactate. The carbonic acid arises by hydration of CO2 formed by oxidation in the TCA cycle, whereas lactic acid is the product of the glycolytic pathway in the absence of oxygen. Excess lactate is exported via monocarboxylate transporters, MCT-1, -2, and sometimes -4, which can also carry H+. Protons themselves are exported via a number of transport systems such as Na+/H+ exchange (NHE), vacuolar H+ ATPases and Na+/HCO3- exchanges. All three systems perform redundant functions and can substitute for one another in the presence of inhibitors. Oxidatively produced CO2 can exit the cell through aquaporins, where it is hydrated by membrane-bound carbonic anhydrases, to yield bicarbonate and a hydrogen ion.

FIGURE 1. Glucose metabolism in mammalian cells.

FIGURE 1

Afferent blood delivers glucose and oxygen (on haemoglobin) to tissues, where it reaches cells by diffusion. Glucose is taken up by specific transporters, where it is converted first to glucose-6-phosphate by hexokinase and then to pyruvate, generating 2 ATP per glucose. In the presence of oxygen, pyruvate is oxidized to HCO3, generating 36 additional ATP per glucose. In the absence of oxygen, pyruvate is reduced to lactate, which is exported from the cell. Note that both processes produce hydrogen ions (H+), which cause acidification of the extracellular space. HbO2, oxygenated haemoglobin. (Ref. 1). Reprinted with permission from NPG.

Maintenance of acid-base homeostasis is critical. However this balance in solid tumors is vulnerable. In tumor cells, the increased glucose catabolism results in significant production of lactate and H+. Although tumor cells have increased acid production, they maintain a normal or alkaline pHi relative to normal cells. The major acid load is transported outside the cells, which cannot be removed by the vasculature. The capacity of primary extracellular buffer is limited; as a result extracellular space becomes acidic. Tumor cells seem well adapted to acidic microenvironments. In fact, in vitro studies have shown that maximum tumor cell proliferation occurs at a pHe of 6.8 instead of 7.3 in normal cells. The excess H+ ions diffuse along concentration gradients from the tumor into adjacent normal tissue resulting in a chronically acidic microenvironment for neighboring normal cells. Recent therapeutic approaches have been designed to target the tumor pH either through low pH activation of pro-drugs, low pH activated release of drug from micelles and nanoparticles, or by drugs that raise pH of acidic tumors. Thus, it will become increasingly important to be able to measure pH with accuracy, precision and high spatio-temporal resolution in experimental preclinical systems as well as in human beings.

PET

PET has been used for measuring tissue pH since 1970s. Techniques used with moderate success employ the distribution of radio-labeled DMO, which distribute according to the pH gradient across semi-permeable membranes via ‘ion trapping’. Although this represents the first noninvasive in vivo pH measurement, it is inaccurate and imprecise, since DMO distribution depends on the plasmalemmal pH gradient and the fractional volumes of intra- and extracellular space, both of which are unknown. Recently, an innovative technique was discovered to selectively target acidic tissues in vivo using pH low insertion peptide (pHLIP), a peptide that predominantly inserts across a lipid bilayer as a monomeric alpha-helix at acidic extracellular environment but not at normal physiological pH. Vāvere, et al., extended this method with PET imaging to investigate the acidic environment in prostate tumors using 64Cu conjugated to the pHLIP (64Cu-DOTA-pHLIP) (2). This is the first time a pHe-sensitive peptide based PET agent has been reported for the delineation of the pHe of tumors. Although the affinity of pHLIP to cell membrane is low at normal physiologic pH, it may result in an inaccurate pHe measurement.

MRS and MRI

In vivo MRS and MRI have been used for more than three decades to monitor metabolic and physiologic processes. Both endogenous and exogenous NMR-active compounds have been used to measure pH in vivo (3). MRS methods are generally based on a difference in chemical shifts between pH-dependent and independent resonances. A number of isotopes have been evaluated to determine tissue pH with MRS. 31P-MRS provides a robust technique for simultaneously measuring pHi from the chemical shift of endogenous inorganic phosphate (Pi) and pHe from the chemical shift of exogenous indicators, such as 3-aminopropyl phosphonate (3-APP). An improvement measurement was achieved using 1H-MRS with pH-sensitive H2 resonance of 2-imidazole-1-yl-3-ethoxycarbonyl propionic acid (IEPA). Although these studies showed that the tumors’ pHe was heterogeneous, they are still limited in spatial and temporal resolution.

Hyperpolarized 13C bicarbonate

Carbon-13 is distinct from more commonly used isotopes in that it is only 1.1% naturally abundant. Hence, 13C studies rely on using compounds with isotopic enrichment. Additionally, Dynamic Nuclear Hyperpolarization (DNP) can radically improve the sensitivity of in vivo 13C MR. The technique is based on transferring the polarization of unpaired electrons to neighboring nuclei by microwave irradiation of the sample. DNP has been shown to be capable of enhancing the MR signal of 13C NMR by more than a factor of 40,000. Brindle and coworkers have recently measured tumor pH using hyperpolarized 13C bicarbonate (4). This measurement used the Henderson-Hasselbalch equation to estimate tissue pH from the voxel-wise ratio of H13CO3- to 13CO2 following injection of hyperpolarized H13CO3-. The results showed that the pH of a lymphoma xenograft was significantly lower (6.7±0.1) than the normal tissue (7.1±0.1). Although a rapid pharmacokinetic distribution of bicarbonate measures a weighted average of pHi and pHe, the results appear weighted to pHe. A limitation of DNP is that the hyperpolarized nuclear spin signal decreases rapidly according to spin-lattice relaxation, T1. Therefore, measurements must be completed within 1-2 minutes following injection. Rapid relaxation also severely restricts the number of phase encoding steps during short acquisition times, resulting in limited spatial resolution. However, fast imaging techniques such as compressed sensing reconstruction can be used to overcome these potential pitfalls (5).

MR relaxometry

An alternative approach using MRI relies on perturbing the relaxivity of water via pH-dependent relaxation agents. A small molecule approach to measure pH has been developed by Sherry and Aime (6-7), who have synthesized gadolinium-based agents whose relaxivity is pH-dependent. In the case of the tetraphosphonate, Gd-DOTA-4AmP5-, the H-bonding network created by phosphonate side-arm protonation provides a catalytic pathway for hydrogen exchange. For quantification, this approach requires accurate knowledge of the agent concentration in each voxel. Raghunand solved this using sequential injection of two gadolinium agents, one of which was pH-insensitive. This has been applied to imaging pH in kidneys and in rat brain glioma (8). In the glioma model, the comparison of pHe and tumor perfusion time-to-maximal amplitude (TMI) indicated that volumes with slower perfusion were correlated with lower pHe values.

Although this method worked well, there are drawbacks to the successive injection of two different agents, especially for potential clinical use. During the course of the injections, prolonged exposure to anesthesia may alter the blood pressure, which can result in significant differences in pharmacokinetics of successive injections. In addition, it is necessary to wait until most of the first agent has exited the tumor before administering the second.

Recently, a relaxivity-based single injection method has been developed, which consists of a mixture Dy-DOTP5- with Gd-DOTA-4AmP5- (9). While the effects of the Gd-contrast agent (CA) on T1 and T2 relaxation exhibited similar pHe-dependence, the Dy-CA induced a strong outer sphere effect on T2* that is pHe-independent with negligible effect on the T1. This method involved measurement of concentration of Dy-CA ([Dy-CA]) through its effects on ΔR2* and subsequently extrapolating the [Gd-CA] from the known mole ratio of Dy- and Gd-CA, thus enabling dynamic calculation of spatially localized unique pHe values. The protocol is outlined in FIGURE 2 and represents the first application of a CA cocktail for the determination of spin lattice and susceptibility induced transverse relaxation in this manner (9). The primary advantage of this protocol over previous studies is the rapidity of the pHe measurement, as high resolution pHe maps can be obtained with ca. 0.20 mM Gd-DOTA-4AmP5-, within 16 minutes after injection. Recently, Aime and colleagues created a peptide that changes between a helix and a random coil in pH-dependent manner, which affects rotational correlation time and T1 relaxivity, but has little effect on T2 relaxivity. This approach consists of measuring the ratio between T1 and T2 paramagnetic contribution to the water protons relaxation rate, which provides an opportunity to measure pH in a concentration-independent fashion (10). In principle, single injection method is capable of yielding pHe maps within practical times in a clinical setting.

FIGURE 2. A schematic overview of the Single Injection Protocol.

FIGURE 2

In vitro calibrations (upper panel) are used to define a relationship between the molar relaxivity of GdDOTA-4AmP5- and pH. In vivo calibrations (lower panel) involve co-injection of pH-independent GdDTPA and DyDOTP. These data are used to define an in vivo relationship between [Gd-CR] and the EPSI-measured line-width. In the experiment, the line-width induced by the co-injected [Dy-CR] is used to calculate the per-pixel [Gd-DOTA-4AmP5-], which is then combined with T1 values to calculate a molar relaxivity and hence, pH. (Ref. 9)

Chemical Exchange Saturation Transfer (CEST)

Compared to T1 and T2 based contrast agents, novel agents have been developed to generate contrast via CEST, particularly at high magnetic fields. The dynamic process of CEST can be described by a simple two pool chemical exchange model, wherein the magnetizations for a labile proton and bulk water are derived by two groups of Bloch equations coupled by chemical exchange. CEST is mediated by pre-saturation of a resonance that is undergoing chemical exchange and measuring the effect on decreasing the abundant water signal. Besides general MRI parameters, exchangeable site concentrations, temperature, and endogenous tissue properties, CEST contrast also depends on pH. In general, the exchange rate is slower at low pH than at high pH due to base catalysis of proton exchange. There are three main categories of CEST imaging: diamagnetic CEST (DIACEST), paramagnetic CEST (PARACEST) and amide proton transfer (APT). Wolff and Balaban first demonstrated the possibility of CEST imaging in which RF saturation was transferred from exchangeable solute protons to water (11). This resulted in further work characterizing the DIACEST pH measurements using high concentrations of two low molecular weight solutes as tracers in vivo. Recently, Aime and colleagues demonstrated that iopamidol can be used as a DIACEST agent for MRI to measure pH in a concentration-independent fashion, because iopamidol contains two chemical groups that have different pH-dependent CEST effects (12). Mori, van Zijl and colleagues optimized methods to obtain accurate chemical exchange rates between water and -NH protons in vivo by avoiding magnetization transfer signal losses for solvent suppression. This has led to characterization of amide proton transfer (APT) effects based on the magnetization exchange from labile endogenous amide protons to bulk water, which has been applied to humans (13). A limitation of CEST imaging is that it requires very homogeneous magnetic fields which are difficult to achieve in motile tissues. However, recent technologies allow voxel-by-voxel correction based on the fact that the CEST spectral width is independent on field inhomogeneity and that the CEST spectrum is only shifted.

The applications of the CEST technique have been furthered by incorporating a paramagnetic center in the exchanging molecule, leading to increased chemical shift dispersions and hence, increased sensitivities (14). Paramagnetic agents with enlarged chemical shifts (of >50 ppm) provide the possibility keeping the slow NMR conditions at very high exchange rates. Lanthanide-based paramagnetic complexes containing both highly shifted pH-insensitive and pH-sensitive exchangeable protons have been developed, wherein the CEST effects at two resonances can be used for a ratiometric determination of pH. Drawback to CEST and PARACEST remain the high concentrations required (>10 mM) and the need for strong MR irradiation pulses for pre-saturation, which are limited by power deposition limitations, or SAR. Pagel’s group has recently developed a new PARACEST agent, Yb-DO3A-oAA, with two pH-responsive CEST effects that have different MR frequencies and different dependencies on pH (15) (FIGURE 3). The ratio of the two PARACEST effects can measure the entire physiological range of pHe from 6.1-8.0 with acceptable RF powers.

FIGURE 3. pHe map of a mouse tumor model.

FIGURE 3

pH was measured by PARACEST MRI with contrast agent Yb-DO3A-oAA. (Data courtesy M Pagel, Ref. 15)

Optics

Optics is another powerful tool of noninvasive pH measurement in tumor and surrounding tissue. The varying fluorescent properties of the probes, which are associated with local pH, can be measured optically and be converted to pH distribution accordingly. Currently, there are two main ways for measuring tumor pH: fluorescence ratio imaging microscopy (FRIM), and fluorescence lifetime imaging microscopy (FLIM), which are accomplished by the measurements of emission spectra and lifetimes of fluorophores, respectively. In fluorescence ratiometric imaging, the emission spectra of some pH probes undergo a pH-dependent wavelength shift, thus allowing the ratio of the fluorescence intensities from the dyes at two emission wavelengths to be used for accurate determinations of pH. However, the association of pH indicators to intracellular proteins and cytosolic constituents was found to modify the ratio of intensities in two emission bands. Moreover, FRIM is based on fluorescence amplitude methods and is thus susceptible to photobleaching and to variation in light scattering and absorption of the sample, which may also introduce the bias in the results of pH measurement. FLIM is an experimental technique in which the fluorescence decay is measured at each spatially resolvable location within a fluorescence image. The pH probes used in FLIM display a pH-dependent shift in fluorescence lifetimes, which can be converted to pH map of tumor accordingly with construction of proper calibration curves. Fluorescence lifetime techniques are generally classified into two types: time-domain and frequency-domain. Compared to frequency-domain methods, time-domain measurements have higher signal-to-noise ratio (SNR) and are widely used for pH imaging (16). Although lifetime-based pH imaging has often been found to be more convenient than conventional ratiometric methods due to a simpler pH calibration, it was pointed out that this method is not necessarily a straightforward approach to measure pH in the absence of correction for the effect of probe binding.

Summary

Techniques for measuring the pH of organelles, cytosol and extracellular fluid in vivo have been consistently improving and converging. Optical techniques based on expression of pH-sensitive fluorescent dye are revolutionizing pH measurements in vitro. With improved detection platforms, optical methods hold promise to be applied in vivo. MR techniques have been developed to measure pHi with endogenous indicators, albeit with low sensitivity. Methods based on exogenous compounds have clearly shown that high resolution and highly sensitivity measurements of pHe (and possibly pHi) are tractable in vivo. Hyperpolarized 13C-labelled bicarbonate technique may potentially be used in the clinic and new generations of pH-sensitive PET tracers are under improvement. All of these developments are a testament to the emerging view that tissue pH is a biomedically important parameter of tumor metabolism.

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