🇮🇳 GATE Biomedical Engineering · subject

GATE Biomedical Engineering Medical Imaging Systems Syllabus

The Medical Imaging Systems syllabus for GATE Biomedical Engineering in full: 2 chapters and 7 topics, every one listed below, plus 50 Medical Imaging Systems flashcards with answers.

2Chapters
7Topics
50Flashcards

Medical Imaging Systems syllabus: all 2 chapters

Expand any chapter to see its topics and sub-topics.

  1. Basic Physics

    1 topic
    • Fundamentals of Physics in Medical Imaging
  2. Instrumentation and Image Formation Techniques

    6 topics
    • X-Ray Imaging
    • Computed Tomography (CT)
    • Single Photon Emission Computed Tomography (SPECT)
    • Positron Emission Tomography (PET)
    • Magnetic Resonance Imaging (MRI)
    • Ultrasound Imaging

GATE Biomedical Engineering Medical Imaging Systems flashcards — 50 questions with answers

  1. What physical quantity defines the energy of an X-ray or gamma photon in terms of its frequency, and what is the governing equation?

    Photon energy is proportional to frequency: $E = h\nu = \frac{hc}{\lambda}$, where $h$ is Planck's constant ($6.626\times10^{-34}\,\text{J·s}$), $\nu$ is frequency, $c$ is the speed of light, and $\lambda$ is wavelength.

  2. State the Beer-Lambert law of attenuation for a monoenergetic X-ray beam passing through a homogeneous medium.

    $I = I_{0}\,e^{-\mu x}$, where $I_{0}$ is incident intensity, $I$ is transmitted intensity, $\mu$ is the linear attenuation coefficient, and $x$ is the thickness traversed.

  3. Define the half-value layer (HVL) and give its relation to the linear attenuation coefficient $\mu$.

    HVL is the thickness of material that reduces beam intensity to half its original value: $\text{HVL} = \frac{\ln 2}{\mu} = \frac{0.693}{\mu}$.

  4. What is the difference between the linear attenuation coefficient and the mass attenuation coefficient?

    The mass attenuation coefficient is the linear coefficient normalized by density: $\frac{\mu}{\rho}$. It removes the dependence on physical density, so $\mu = \left(\frac{\mu}{\rho}\right)\rho$, with units $\text{cm}^{2}/\text{g}$.

  5. Name the three primary photon interaction mechanisms relevant to diagnostic medical imaging and their approximate energy dominance.

    Photoelectric effect (dominates at low energies, strong $Z$ dependence), Compton scattering (dominates at diagnostic/intermediate energies), and pair production (only above $1.022\,\text{MeV}$, not used in diagnostics).

  6. How does the photoelectric effect's probability depend on atomic number $Z$ and photon energy $E$?

    The photoelectric cross-section scales approximately as $\frac{Z^{3\text{–}4}}{E^{3}}$, making it strongly dependent on atomic number and dominant at low energies — the basis of high-contrast bone imaging.

  7. In Compton scattering, what is the Compton wavelength shift equation for a photon scattered at angle $\theta$?

    $\Delta\lambda = \lambda' - \lambda = \frac{h}{m_{e}c}\,(1 - \cos\theta)$, where $\frac{h}{m_{e}c} \approx 2.43\times10^{-12}\,\text{m}$ is the Compton wavelength of the electron.

  8. What are the two main processes by which X-rays are produced in an X-ray tube?

    Bremsstrahlung (braking radiation, producing a continuous spectrum as electrons decelerate near nuclei) and characteristic radiation (discrete lines from electron transitions filling inner-shell vacancies).

  9. In an X-ray tube, how does the maximum (cutoff) photon energy relate to the applied tube voltage?

    The maximum photon energy equals the kinetic energy of the accelerated electrons: $E_{\max} = eV$, so the minimum wavelength is $\lambda_{\min} = \frac{hc}{eV}$ (Duane–Hunt law).

  10. What is the role of filtration (e.g., aluminium) in an X-ray tube?

    Filtration preferentially removes low-energy (soft) photons that would only add patient dose without contributing to the image, hardening the beam and raising its mean energy.

  11. Define radiographic contrast and list the main factors that affect it.

    Radiographic contrast is the difference in optical density (or signal) between adjacent regions of an image. It depends on subject contrast (differences in $\mu$, thickness, density), kVp (lower kVp = higher contrast), and scatter radiation (which reduces contrast).

  12. What is the purpose of an anti-scatter grid in projection radiography?

    An anti-scatter grid absorbs Compton-scattered photons before they reach the detector, improving image contrast at the cost of increased patient dose (requiring higher exposure).

  13. Define the SI units becquerel (Bq), gray (Gy), and sievert (Sv).

    Becquerel = 1 nuclear disintegration per second (activity). Gray = $1\,\text{J/kg}$ of absorbed dose. Sievert = equivalent/effective dose = absorbed dose × radiation weighting factor, accounting for biological effect.

  14. What is the fundamental relationship between projection data and the imaged object in computed tomography?

    Each CT projection is a line integral of the attenuation coefficient along the X-ray path: $p(s,\theta) = \int \mu(x,y)\,dl$. The full set of projections over angles is the Radon transform of $\mu(x,y)$.

  15. How are CT numbers (Hounsfield Units) defined?

    $\text{HU} = 1000 \times \frac{\mu_{\text{tissue}} - \mu_{\text{water}}}{\mu_{\text{water}}}$. By definition water = $0\,\text{HU}$ and air $\approx -1000\,\text{HU}$.

  16. What are the approximate Hounsfield Unit values for air, water, fat, and dense bone?

    Air $\approx -1000\,\text{HU}$, fat $\approx -100\,\text{to}\,-50\,\text{HU}$, water $= 0\,\text{HU}$, soft tissue $\approx +40\,\text{HU}$, dense/cortical bone $\approx +1000\,\text{HU}$ or higher.

  17. Name the standard image reconstruction algorithm in CT and state the role of the filter (kernel).

    Filtered back-projection (FBP). The projections are convolved with a ramp filter ($|f|$ in the frequency domain) before back-projection to compensate for the $\frac{1}{r}$ blurring that simple back-projection introduces.

  18. State the Fourier slice (central slice) theorem as used in CT reconstruction.

    The 1-D Fourier transform of a projection taken at angle $\theta$ equals a radial slice, at angle $\theta$, through the 2-D Fourier transform of the object. This links projection data to the object's frequency content.

  19. What distinguishes the successive generations of CT scanner geometry (1st through 4th)?

    1st gen: single pencil beam + single detector, translate–rotate. 2nd gen: narrow fan beam + multiple detectors, translate–rotate. 3rd gen: wide fan beam covering patient, detector and tube rotate together. 4th gen: full stationary detector ring, only the tube rotates.

  20. What is the Nyquist criterion as applied to CT/imaging sampling?

    To avoid aliasing, the sampling frequency must be at least twice the highest spatial frequency present: $f_{s} \geq 2 f_{\max}$. Equivalently, sample spacing must be $\leq \frac{1}{2f_{\max}}$.

Show the other 30 Medical Imaging Systems flashcards
  1. In nuclear medicine, what defines an ideal radiotracer for SPECT imaging?

    It should emit gamma photons of suitable energy (~$100\text{–}200\,\text{keV}$) for detection, have a short physical half-life, pure gamma emission (no particulate radiation adding dose), and selective biological uptake in the target tissue.

  2. What is the most commonly used radionuclide in SPECT, its gamma energy, and physical half-life?

    Technetium-99m ($\ce{^{99m}Tc}$), which emits gamma photons of about $140\,\text{keV}$ and has a physical half-life of approximately $6\,\text{hours}$.

  3. Describe the basic detector components of a gamma (Anger) camera used in SPECT.

    A collimator (defines direction), a large scintillation crystal (usually NaI(Tl)) that converts gammas to light, an array of photomultiplier tubes (PMTs), and position/energy logic circuitry (Anger logic) to compute event location and reject scatter via a pulse-height window.

  4. Why does a gamma camera require a physical collimator while a CT scanner does not?

    Gamma photons are emitted isotropically from inside the patient with no inherent directional information, so a lead collimator is needed to accept only photons traveling along defined directions. CT uses an external, directional X-ray source, so geometry is known.

  5. State the law of radioactive decay and define the decay constant $\lambda$.

    $N(t) = N_{0}\,e^{-\lambda t}$, where $\lambda$ is the decay constant (probability of decay per unit time). The half-life is $T_{1/2} = \frac{\ln 2}{\lambda} = \frac{0.693}{\lambda}$.

  6. Define effective half-life and give its formula in terms of physical and biological half-lives.

    Effective half-life accounts for both radioactive decay and biological clearance: $\frac{1}{T_{\text{eff}}} = \frac{1}{T_{\text{phys}}} + \frac{1}{T_{\text{bio}}}$.

  7. What is the fundamental physical principle that distinguishes PET from SPECT?

    PET uses positron-emitting radionuclides; an emitted positron annihilates with an electron, producing two $511\,\text{keV}$ gamma photons emitted ~$180^{\circ}$ apart. Detection relies on coincidence detection of these photon pairs rather than physical collimation.

  8. What is the energy of each annihilation photon in PET, and why is this value fixed?

    Each photon has energy $511\,\text{keV}$, equal to the rest-mass energy of the electron/positron: $E = m_{e}c^{2} = 0.511\,\text{MeV}$. Two are produced to conserve energy and momentum.

  9. Define a 'line of response' (LOR) in PET and explain electronic (coincidence) collimation.

    A line of response is the straight line connecting two detectors that register annihilation photons within a short coincidence timing window. Because the line is defined electronically by simultaneous detection, no physical collimator is needed — this is electronic collimation.

  10. Name the most widely used PET radiotracer and the metabolic process it images.

    Fluorine-18 fluorodeoxyglucose ($\ce{^{18}F}$-FDG), a glucose analogue. It images glucose metabolism, with high uptake in metabolically active tissues such as many tumors and the brain.

  11. What is time-of-flight (TOF) PET and what advantage does it provide?

    TOF PET measures the small difference in arrival times of the two annihilation photons to localize the annihilation point along the line of response, improving signal-to-noise ratio and image quality.

  12. Why does PET generally offer better spatial resolution and sensitivity than SPECT?

    PET uses electronic coincidence detection (no absorptive collimator, so far higher sensitivity) and the back-to-back $511\,\text{keV}$ photons define lines of response precisely, giving better resolution. SPECT's collimator absorbs most photons, lowering sensitivity.

  13. What nuclear property is exploited in magnetic resonance imaging, and which nucleus is primarily imaged?

    Nuclear spin / magnetic moment of nuclei with odd nucleon number. MRI primarily images the hydrogen nucleus ($\ce{^{1}H}$, a single proton) due to its high abundance in water and fat in the body.

  14. State the Larmor equation governing nuclear precession in MRI.

    $\omega_{0} = \gamma B_{0}$ (or $f_{0} = \frac{\gamma}{2\pi}B_{0}$), where $\omega_{0}$ is the Larmor precession frequency, $\gamma$ is the gyromagnetic ratio, and $B_{0}$ is the static magnetic field strength.

  15. What is the gyromagnetic ratio of the hydrogen proton (in MHz/T)?

    $\frac{\gamma}{2\pi} \approx 42.58\,\text{MHz/T}$ for $\ce{^{1}H}$. Thus at $1.5\,\text{T}$ the Larmor frequency is about $63.9\,\text{MHz}$.

  16. Define T1 (longitudinal/spin-lattice) relaxation in MRI.

    T1 is the time constant for recovery of longitudinal magnetization $M_{z}$ toward equilibrium after an RF pulse, via energy exchange with the surrounding lattice: $M_{z}(t) = M_{0}\left(1 - e^{-t/T_{1}}\right)$.

  17. Define T2 (transverse/spin-spin) relaxation in MRI.

    T2 is the time constant for decay of transverse magnetization $M_{xy}$ due to loss of phase coherence among spins: $M_{xy}(t) = M_{0}\,e^{-t/T_{2}}$. T2 is always $\leq$ T1.

  18. Distinguish T2 from T2* relaxation.

    T2 results from intrinsic spin-spin interactions. T2* includes additional dephasing from static magnetic field inhomogeneities: $\frac{1}{T_{2}^{*}} = \frac{1}{T_{2}} + \frac{1}{T_{2,\text{inhomo}}}$, so $T_{2}^{*} \leq T_{2}$. Spin-echo recovers T2; gradient-echo reflects T2*.

  19. What are the roles of repetition time (TR) and echo time (TE) in MRI image weighting?

    TR is the time between successive RF excitation pulses; TE is the time from excitation to echo readout. Short TR + short TE = T1-weighted; long TR + long TE = T2-weighted; long TR + short TE = proton-density-weighted.

  20. What is the function of magnetic gradient coils in MRI?

    Gradient coils superimpose linear spatial variations on $B_{0}$ so the Larmor frequency becomes position-dependent. They enable slice selection, frequency encoding, and phase encoding — i.e., spatial localization of the signal.

  21. What is k-space in MRI and how is the image obtained from it?

    k-space is the spatial-frequency (Fourier) domain where raw MRI data are acquired, with axes determined by phase- and frequency-encoding gradients. The image is reconstructed by applying a 2-D (inverse) Fourier transform to the k-space data.

  22. What is the fundamental relationship between ultrasound propagation speed, frequency, and wavelength?

    $c = f\lambda$, where $c$ is the speed of sound in the medium (~$1540\,\text{m/s}$ in soft tissue), $f$ is frequency, and $\lambda$ is wavelength. Higher frequency gives shorter wavelength and better resolution but less penetration.

  23. Define acoustic impedance and give its equation.

    Acoustic impedance is $Z = \rho c$, the product of medium density $\rho$ and sound speed $c$ (units rayl, $\text{kg·m}^{-2}\text{s}^{-1}$). Differences in $Z$ at interfaces determine the strength of ultrasound reflections (echoes).

  24. What fraction of ultrasound intensity is reflected at a boundary between two media of impedance $Z_{1}$ and $Z_{2}$?

    The pressure reflection coefficient is $R = \frac{Z_{2} - Z_{1}}{Z_{2} + Z_{1}}$, and the intensity reflection coefficient is $R_{I} = \left(\frac{Z_{2} - Z_{1}}{Z_{2} + Z_{1}}\right)^{2}$.

  25. What physical effect underlies ultrasound transducers, and what material is commonly used?

    The piezoelectric effect: a material (commonly lead zirconate titanate, PZT) deforms under an applied voltage to generate sound and produces a voltage when deformed by returning echoes, enabling it to both transmit and receive ultrasound.

  26. How is depth (range) of a reflector determined in pulse-echo ultrasound?

    From the round-trip echo time $t$: $d = \frac{c\,t}{2}$, where $c$ is the speed of sound and the factor $\frac{1}{2}$ accounts for the sound traveling to the reflector and back.

  27. State the Doppler equation used in ultrasound to measure blood flow velocity.

    $f_{d} = \frac{2 f_{0} v \cos\theta}{c}$, where $f_{d}$ is the Doppler frequency shift, $f_{0}$ the transmitted frequency, $v$ the reflector velocity, $\theta$ the angle between the beam and flow, and $c$ the speed of sound.

  28. Compare A-mode, B-mode, and M-mode ultrasound display formats.

    A-mode (amplitude): 1-D plot of echo amplitude vs depth. B-mode (brightness): 2-D grayscale image where echo amplitude maps to pixel brightness. M-mode (motion): displays the motion of a structure along one line over time, used for moving structures like heart valves.

  29. What is time-gain compensation (TGC) in ultrasound, and why is it needed?

    TGC progressively amplifies echoes returning from greater depths to compensate for attenuation of the beam as it travels deeper into tissue, producing uniform image brightness regardless of reflector depth.

  30. Summarize the key trade-off between ionizing and non-ionizing modalities by classifying CT, PET, SPECT, MRI, and ultrasound.

    Ionizing (use radiation, dose concern): X-ray, CT, SPECT, PET — CT/X-ray give anatomy, SPECT/PET give functional/metabolic information. Non-ionizing (no radiation dose): MRI (superb soft-tissue contrast, anatomy + function) and ultrasound (real-time, portable, no dose, operator-dependent).

GATE Biomedical Engineering Medical Imaging Systems FAQ

What is in the GATE Biomedical Engineering Medical Imaging Systems syllabus?

GATE Biomedical Engineering Medical Imaging Systems is split into 2 chapters: Basic Physics and Instrumentation and Image Formation Techniques. Together they contain 7 topics.

How many chapters are in GATE Biomedical Engineering Medical Imaging Systems?

2 chapters, containing 7 topics. The largest chapter is Instrumentation and Image Formation Techniques, with 6 topics.

Are there flashcards for GATE Biomedical Engineering Medical Imaging Systems?

Yes — a 50-card Medical Imaging Systems deck, printed in full in the flashcards section of this page and available in the Examius app with spaced repetition. The free plan covers one exam of your choice, including its flashcards; Examius Pro, a one-time purchase, unlocks every other exam and deck.