Give step-by-step solution with explanation and final answer:In many MR experiments it is necessary to flip a spin which is initially aligned along the z axis
into the X’-y’ plane by using an appropriate rotating magnetic field B1 during a certain amount of
time (pulse) (in the rotating frame, Bl is a static field orthogonal to BO). This is referred to as a 90
degrees pulse. If the desired pulse time is 1.0 ms, what B1 magnitude is required for
a. A proton spin?
b. A carbon spin?
c. At which frequency are rotating magnetizations originating from these two atoms?
d. AtaBo of 5 T, at which frequency must B, rotate (in the lab frame) in resonance
conditions for a proton spin?
e. What is then the wavelength and energy of a photon of this field? Compare it to what is
used of X-ray imaging.
Question:
Give step-by-step solution with explanation and final answer:In many MR experiments it is necessary to flip a spin which is initially aligned along the z axis
into the X’-y’ plane by using an appropriate rotating magnetic field B1 during a certain amount of
time (pulse) (in the rotating frame, Bl is a static field orthogonal to BO). This is referred to as a 90
degrees pulse. If the desired pulse time is 1.0 ms, what B1 magnitude is required for
a. A proton spin?
b. A carbon spin?
c. At which frequency are rotating magnetizations originating from these two atoms?
d. AtaBo of 5 T, at which frequency must B, rotate (in the lab frame) in resonance
conditions for a proton spin?
e. What is then the wavelength and energy of a photon of this field? Compare it to what is
used of X-ray imaging.
This is AI generated Response.
Asked by: hhhh
Created at: 2025-05-28 08:16:28
Final Answer:
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Let's solve each part step-by-step:
---
### **Given Data**
- 90° pulse time (\( t_{90} \)) = 1.0 ms = \(1.0 \times 10^{-3}\) s
- \( B_0 = 5\,T \) (for part d)
- For 90° pulse: The magnetization must rotate by π/2 radians.
- Gyromagnetic ratio (\( \gamma \)):
- Proton (\( ^1H \)): \( \gamma_p = 2.675 \times 10^8\, \text{rad/s/T} \)
- Carbon-13 (\( ^{13}C \)): \( \gamma_c = 6.728 \times 10^7\, \text{rad/s/T} \)
---
## **a. B1 Magnitude for a Proton Spin**
For a 90° pulse:
\[
\theta = \gamma B_1 t_{p}
\]
For 90° (\( \theta = \frac{\pi}{2} \)) and \( t_{p} = 1.0 \) ms:
\[
\frac{\pi}{2} = \gamma_p B_1 t_p
\]
\[
B_1 = \frac{\pi}{2\gamma_p t_p}
\]
Plug in the values:
\[
B_1 = \frac{\pi}{2 \cdot (2.675 \times 10^8) \cdot (1.0 \times 10^{-3})}
\]
\[
B_1 = \frac{3.1416}{2 \cdot 2.675 \times 10^5}
\]
\[
B_1 = \frac{3.1416}{5.35 \times 10^5}
\]
\[
B_1 \approx 5.88 \times 10^{-6}\, \text{T} = 5.88\, \mu\text{T}
\]
---
## **b. B1 Magnitude for a Carbon Spin**
Use the same formula but with \( \gamma_c \):
\[
B_1 = \frac{\pi}{2 \gamma_c t_p}
\]
\[
B_1 = \frac{3.1416}{2 \cdot 6.728 \times 10^7 \cdot 1.0 \times 10^{-3}}
\]
\[
B_1 = \frac{3.1416}{1.3456 \times 10^5}
\]
\[
B_1 \approx 2.34 \times 10^{-5}\, \text{T} = 23.4\, \mu\text{T}
\]
---
## **c. Larmor Frequency for Protons and Carbons**
Larmor frequency:
\[
f = \frac{\gamma}{2\pi} B_0
\]
For protons (\( \gamma_p \)):
\[
f_p = \frac{2.675 \times 10^8}{2\pi} \cdot 5
\]
\[
f_p \approx 4.257 \times 10^7 \cdot 5 = 2.1285 \times 10^8\, \text{Hz} = 212.85\, \text{MHz}
\]
For carbon-13 (\( \gamma_c \)):
\[
f_c = \frac{6.728 \times 10^7}{2\pi} \cdot 5
\]
\[
f_c \approx 1.072 \times 10^7 \cdot 5 = 5.36 \times 10^7\, \text{Hz} = 53.6\, \text{MHz}
\]
---
## **d. Frequency Needed for Resonance for Protons at \( B_0 = 5\,T \)**
Already calculated above:
\[
f_p = 212.85\, \text{MHz}
\]
---
## **e. Wavelength and Energy of a Photon of This Field**
Wavelength (\( \lambda \)):
\[
\lambda = \frac{c}{f}
\]
where \( c = 3.00 \times 10^8\, \text{m/s} \).
\[
\lambda = \frac{3.00 \times 10^8}{2.1285 \times 10^8}
\]
\[
\lambda \approx 1.41\, \text{m}
\]
Energy (\( E \)):
\[
E = h f
\]
where \( h = 6.626 \times 10^{-34}\, \text{J s} \).
\[
E = 6.626 \times 10^{-34} \cdot 2.1285 \times 10^8
\]
\[
E \approx 1.41 \times 10^{-25}\, \text{J}
\]
### **Compare to X-rays**
- X-ray energies: \( \sim 10^{-16} \) to \( 10^{-15} \) J (tens of keV)
- X-ray wavelengths: \( \sim 10^{-10} \) m (angstrom scale)
**Conclusion:** MRI photons are much lower in energy and much longer in wavelength than X-rays.
---
## **Summary Table**
| Part | Calculation | Value |
|------|-------------|-------|
| a | \( B_1 \) for proton | \( 5.88\, \mu\text{T} \) |
| b | \( B_1 \) for carbon | \( 23.4\, \mu\text{T} \) |
| c | Larmor freq (proton) | \( 212.85\, \text{MHz} \) |
| | Larmor freq (carbon) | \( 53.6\, \text{MHz} \) |
| d | Resonance freq (proton, 5 T) | \( 212.85\, \text{MHz} \) |
| e | Wavelength (proton, 5 T) | \( 1.41\, \text{m} \) |
| | Energy (photon, proton, 5 T) | \( 1.41 \times 10^{-25}\, \text{J} \) |
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