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Thermodynamics question

2025 · 29 Jan · Shift 1 · Q5
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  5. /2025 · 29 Jan · Shift 1 · Q5

Thermodynamics question

2025 · 29 Jan · Shift 1 · Q5

JEE MainChemistryThermodynamicsMCQ+4 / −1
500 J of energy is transferred as heat to 0.5 mol of Argon gas at 298 K and 1.00 atm. The final temperature and the change in internal energy respectively are: Given: R = 8.3 J K-1 mol-1
  1. A
    368 K and 500 J
  2. B
    348 K and 300 J
  3. C
    378 K and 300 J
  4. D
    378 K and 500 J
View written solutionFree

Correct answer: B

  1. Identify the process

The gas is heated at constant pressure because the initial pressure is given as 1.00 atm1.00\,\text{atm}1.00atm and the standard interpretation here is heating under constant atmospheric pressure.

Given:

  • Heat supplied: q=500 Jq = 500\,\text{J}q=500J
  • Moles of Ar: n=0.5n = 0.5n=0.5 mol
  • Initial temperature: T1=298 KT_1 = 298\,\text{K}T1​=298K
  • Argon is a monoatomic ideal gas
  1. Use molar heat capacity at constant pressure

For a monoatomic ideal gas, CV,m=32R,CP,m=CV,m+R=52RC_{V,m} = \frac{3}{2}R, \qquad C_{P,m} = C_{V,m}+R = \frac{5}{2}RCV,m​=23​R,CP,m​=CV,m​+R=25​R

So, CP,m=52(8.3)=20.75 J mol−1K−1C_{P,m} = \frac{5}{2}(8.3) = 20.75\,\text{J mol}^{-1}\text{K}^{-1}CP,m​=25​(8.3)=20.75J mol−1K−1

For 0.50.50.5 mol, nCP=0.5×20.75=10.375 J K−1nC_P = 0.5 \times 20.75 = 10.375\,\text{J K}^{-1}nCP​=0.5×20.75=10.375J K−1

  1. Find temperature rise

At constant pressure, q=nCPΔTq = nC_P\Delta Tq=nCP​ΔT

Thus, ΔT=qnCP=50010.375≈48.2 K\Delta T = \frac{q}{nC_P} = \frac{500}{10.375} \approx 48.2\,\text{K}ΔT=nCP​q​=10.375500​≈48.2K

Therefore, T2=T1+ΔT=298+48.2≈346.2 KT_2 = T_1 + \Delta T = 298 + 48.2 \approx 346.2\,\text{K}T2​=T1​+ΔT=298+48.2≈346.2K

Closest option: T2≈348 KT_2 \approx 348\,\text{K}T2​≈348K

  1. Find change in internal energy

For an ideal gas, ΔU=nCVΔT\Delta U = nC_V\Delta TΔU=nCV​ΔT

Now, CV,m=32R=32(8.3)=12.45 J mol−1K−1C_{V,m} = \frac{3}{2}R = \frac{3}{2}(8.3) = 12.45\,\text{J mol}^{-1}\text{K}^{-1}CV,m​=23​R=23​(8.3)=12.45J mol−1K−1

So for 0.50.50.5 mol, nCV=0.5×12.45=6.225 J K−1nC_V = 0.5 \times 12.45 = 6.225\,\text{J K}^{-1}nCV​=0.5×12.45=6.225J K−1

Hence, ΔU=6.225×48.2≈300 J\Delta U = 6.225 \times 48.2 \approx 300\,\text{J}ΔU=6.225×48.2≈300J

Alternatively, using ΔU=q−PΔV\Delta U = q - P\Delta VΔU=q−PΔV with constant pressure heating of an ideal gas, PΔV=nRΔT=0.5×8.3×48.2≈200 JP\Delta V = nR\Delta T = 0.5 \times 8.3 \times 48.2 \approx 200\,\text{J}PΔV=nRΔT=0.5×8.3×48.2≈200J so ΔU=500−200=300 J\Delta U = 500 - 200 = 300\,\text{J}ΔU=500−200=300J

  1. Match with options

The final temperature and internal energy change are:

  • Final temperature ≈348 K\approx 348\,\text{K}≈348K
  • ΔU≈300 J\Delta U \approx 300\,\text{J}ΔU≈300J

So the correct option is B.

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