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QJEEAdv09Ph4b54: JEE Advanced 2009 Physics - Class 12 JEEAdv09Ph4b54 Solution: Results of calculations for four different designs of a fusion…

Results of calculations for four different designs of a fusion reactor using D-D reaction are given below. Which of these is most promising based on Lawson criterion?

Multiple Choice Options

  • A Deuteron density = 2.0×1012 cm−32.0\times10^{12}~\mathrm{cm^{-3}} ; Confinement time = 5.0×10−3 s5.0\times10^{-3}~\mathrm{s} .
  • B Deuteron density = 8.0×1014 cm−38.0\times10^{14}~\mathrm{cm^{-3}} ; Confinement time = 9.0×10−1 s9.0\times10^{-1}~\mathrm{s} .
  • C Deuteron density = 4.0×1023 cm−34.0\times10^{23}~\mathrm{cm^{-3}} ; Confinement time = 1.0×10−11 s1.0\times10^{-11}~\mathrm{s} .
  • D Deuteron density = 1.0×1024 cm−31.0\times10^{24}~\mathrm{cm^{-3}} ; Confinement time = 4.0×10−12 s4.0\times10^{-12}~\mathrm{s} .

Step-by-Step Verified Solution

To determine the most promising design based on the Lawson criterion, we need to calculate the Lawson number ( nt0nt_0 ) for each design and check if it exceeds 5×10145 \times 10^{14} s/cm 3^3 . We will do this for each of the given options:

Option A:

Deuteron density, n=2.0×1012 cm−3n = 2.0 \times 10^{12}~\mathrm{cm^{-3}}

Confinement time, t0=5.0×10−3 st_0 = 5.0 \times 10^{-3}~\mathrm{s}

Lawson number, nt0=n⋅t0=(2.0×1012)⋅(5.0×10−3)=1.0×1010 s/cm3nt_0 = n \cdot t_0 = (2.0 \times 10^{12}) \cdot (5.0 \times 10^{-3}) = 1.0 \times 10^{10}~\mathrm{s/cm^3}

Option B:

Deuteron density, n=8.0×1014 cm−3n = 8.0 \times 10^{14}~\mathrm{cm^{-3}}

Confinement time, t0=9.0×10−1 st_0 = 9.0 \times 10^{-1}~\mathrm{s}

Lawson number, nt0=n⋅t0=(8.0×1014)⋅(9.0×10−1)=7.2×1014 s/cm3nt_0 = n \cdot t_0 = (8.0 \times 10^{14}) \cdot (9.0 \times 10^{-1}) = 7.2 \times 10^{14}~\mathrm{s/cm^3}

Option C:

Deuteron density, n=4.0×1023 cm−3n = 4.0 \times 10^{23}~\mathrm{cm^{-3}}

Confinement time, t0=1.0×10−11 st_0 = 1.0 \times 10^{-11}~\mathrm{s}

Lawson number, nt0=n⋅t0=(4.0×1023)⋅(1.0×10−11)=4.0×1012 s/cm3nt_0 = n \cdot t_0 = (4.0 \times 10^{23}) \cdot (1.0 \times 10^{-11}) = 4.0 \times 10^{12}~\mathrm{s/cm^3}

Option D:

Deuteron density, n=1.0×1024 cm−3n = 1.0 \times 10^{24}~\mathrm{cm^{-3}}

Confinement time, t0=4.0×10−12 st_0 = 4.0 \times 10^{-12}~\mathrm{s}

Lawson number, nt0=n⋅t0=(1.0×1024)⋅(4.0×10−12)=4.0×1012 s/cm3nt_0 = n \cdot t_0 = (1.0 \times 10^{24}) \cdot (4.0 \times 10^{-12}) = 4.0 \times 10^{12}~\mathrm{s/cm^3}

Based on the calculations, the Lawson numbers for each option are:

  • Option A: 1.0×1010 s/cm31.0 \times 10^{10}~\mathrm{s/cm^3}
  • Option B: 7.2×1014 s/cm37.2 \times 10^{14}~\mathrm{s/cm^3}
  • Option C: 4.0×1012 s/cm34.0 \times 10^{12}~\mathrm{s/cm^3}
  • Option D: 4.0×1012 s/cm34.0 \times 10^{12}~\mathrm{s/cm^3}

The most promising design based on the Lawson criterion, which requires the Lawson number to be greater than 5×1014 s/cm35 \times 10^{14}~\mathrm{s/cm^3} , is Option B because its Lawson number exceeds the threshold.

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