Radiopharmacy

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Radiopharmacy





Introduction


Elements that emit radiation are known as radionuclides and have a number of applications in medicine. Radiopharmacy in hospital practice is concerned with the manufacture or preparation of radioactive medicines known as radiopharmaceuticals. These have two main applications in medicine:



Diagnostic radiopharmaceuticals may be classified into two types:



In diagnostic imaging, gamma-emitting radionuclides are used, since their interaction with tissue is much less than that of particulate emitters and will cause significantly less damage to tissue. Radiopharmaceuticals are administered to the patient, usually by the intravenous (IV) route, and distribute into a particular organ. The radiation is then detected externally using a special scintillation detector known as a gamma-camera. These are used by nuclear medicine departments to image the distribution of the radiopharmaceutical within the patient’s body. Using the gamma-camera in conjunction with a computer system it is not only possible to produce static images of an organ, but also to examine how the radiopharmaceutical moves through an organ. These dynamic images describe how the organ is functioning. It is also possible to create images in three dimensions, a process known as single photon emission computerized tomography (SPECT) when used in combination with gamma-emitting radionuclides such as 99mTc and positron emission tomography (PET) when used in combination with positron-emitting radionuclides such as 18F.


It is important to note that for the safe production of radiopharmaceuticals, the radiopharmacy must be designed to comply with, and procedures must follow, good manufacturing practice and good radiation protection practice. Radiopharmacists working in this field are part of a multidisciplinary team which includes physicians, physicists, radiochemists and technicians from the field of pharmacy as well as nuclear medicine. As part of this team, they not only ensure that the radiopharmaceuticals will give high-quality clinical information, but also that they are safe for both patient and user alike.



Radionuclides used in nuclear medicine




Beta-emitters


Beta-decay occurs in two ways, one that involves the emission of a negatively charged beta-particle, or electron, and the other that involves the emission of a positively charged beta+-particle, or positron.



Beta-emitters


Radionuclides which decay by beta-decay tend to have nuclei that are neutron rich. They attempt to reach a more stable state by the transformation of a neutron into a proton with the emission of a beta -particle (e.g. 32P: 3215P → 3216S + beta). Despite beta-particles having a range in air of up to several metres, their range in tissues is only a few millimetres. Because of this and their highly ionizing nature, beta-emitters tend to be used in therapeutic radiopharmaceuticals (Table 45.1).



The principle of therapeutic treatment with radionuclides is to target the radionuclide to a specific tissue within the body in an attempt to selectively damage or destroy that tissue. Ideally, therapeutic beta-emitting radionuclides should have energies of 0.5–1.5 MeV and a half-life of several days to provide a prolonged radiobiological effect.


The most widely used example of this is 131I- sodium iodide, which is used in the treatment of hyperactive thyroid disease and in certain thyroid tumours. Here the physiological property of thyroid tissue is exploited to target the radionuclide to the site of action. Since thyroid tissue avidly takes up iodine in the normal synthesis of the hormone levothyroxine, radioactive iodine is also taken up and held in the thyroid tissue. Hence, the radiation damage is targeted to the thyroid tissue specifically and the normal excretion of any excess iodine results in no significant damage to other organs and tissues.



Beta+-emitters (positrons)


Radionuclides that emit positrons are becoming more widely used in nuclear medicine. In this transformation, a proton-rich nuclide attempts to achieve stability by converting a proton to a neutron with the emission of a positron (e.g. 11C:116C → 115S + beta+ + gamma). The positron is very short-lived, since it interacts with an electron resulting in an annihilation reaction and the conversion of both particles into electromagnetic (EM) radiation. This EM radiation is in the form of two gamma-rays, each having energy of 0.511 MeV, which are emitted at an angle of 180° to each other.


When used in conjunction with a specialized gamma-camera with detectors placed 180° apart, it is possible to create images in all three dimensions with the position of the radiopharmaceutical being very precisely known. This type of imaging technique is known as positron emission tomography (PET). There are a number of positron emitting radionuclides which are becoming important tools in diagnostic imaging. Currently 18F-labelled glucose, known as 18F-fluoro deoxy-glucose (18F-FDG), is the most commonly used PET radiopharmaceutical in hospital practice and as a result the production processes for it will be described in simplified form and used as an example (see below). However, it should be noted there are four main positron emitters used to prepare radiopharmaceuticals (see Table 45.1). PET imaging with 18F-FDG, in combination with X-ray computerized tomography (CT) is rapidly becoming an important imaging technique in the diagnosis of cancer.




Isomeric transition


Some radionuclides exist for measurable periods in excited, or isomeric, states prior to reaching ground state. This form of decay involves the emission of a gamma-ray and is known as isomeric transition. When radionuclides exist in this transitional state, they are known as metastable, which is denoted by the letter ‘m’ and written thus: 99mTc.


A simplified decay scheme for 99mTc-technetium is shown in Figure 45.1 where 99mTc’s parent radionuclide, molybdenum (99Mo), decays by beta-emission to the ground state 99Tc either directly or indirectly.



The indirect route, which is the most common, involves the isomer 99mTc, which in turn decays from its metastable state to 99Tc by isomeric transition.


Radionuclides which decay by this process are used in diagnostic imaging since they emit gamma-rays (see Table 45.1). It should be noted that 99mTc is the most widely used radionuclide in hospital radiopharmacy today, making up the radionuclide component of around 90% of the radiopharmaceuticals produced. For these reasons the production processes for 99mTc-radiopharmaceuticals will be especially emphasized (see below).



Principles of 99mTc-radiopharmaceutical production


The physical and chemical properties of 99mTc make it nearly ideal for imaging purposes as outlined below:



image It has a 6-h half-life (T1/2); long enough to allow imaging to take place in the working day, while also being short enough that patients are not radioactive for long periods (in 24 h, or 4 half-lives, the radioactivity will have decayed by 94%)


image 99mTc emits gamma-rays of 140 keV energy: ideal for use with the modern gamma-camera


image There are no particulate emissions that, if present, would add to the patient’s radiation dose


image By purchasing a device known as a 99Mo/99mTc -generator, 99mTc can be made readily available to the hospital site in a sterile and pyrogen-free form


image 99mTc has versatile coordination chemistry and will allow a large number of ligands to complex with it. By using different ligands in the radiopharmaceutical’s formulation, a wide range of radiopharmaceuticals can be prepared in the radiopharmacy, providing for the many different investigations carried out in nuclear medicine departments (Table 45.2).


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Jun 24, 2016 | Posted by in PHARMACY | Comments Off on Radiopharmacy

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