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NCERT Exemplar · Q51

Q.Match the following :
Column A

(i) Adiabatic process
(ii) Isolated system
(iii) Isothermal change
(iv) Path function
(v) State function
(vi) ΔU = q
(vii) Law of conservation of energy
(viii) Reversible process
(ix) Free expansion
(x) ΔH = q
(xi) Intensive property
(xii) Extensive property
Column B
(a) Heat
(b) At constant volume
(c) First law of thermodynamics
(d) No exchange of energy and matter
(e) No transfer of heat
(f) Constant temperature
(g) Internal energy
(h) pext = 0
(i) At constant pressure
(j) Infinitely slow process which proceeds through a series of equilibrium states.
(k) Entropy
(l) Pressure
(m) Specific heat
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Each thermodynamic term in Column A pairs with its defining characteristic in Column B. Note that an intensive property matches two entries — both pressure and specific heat are intensive.

Using the definitions from the First Law and the classification of processes, systems and properties, each item matches as follows.

Matching

  1. (i) Adiabatic process → (e) No transfer of heat. An adiabatic process has q=0q = 0; the system is thermally insulated.
  2. (ii) Isolated system → (d) No exchange of energy and matter. Neither energy nor matter crosses the boundary.
  3. (iii) Isothermal change → (f) Constant temperature. ΔT=0\Delta T = 0 throughout.
  4. (iv) Path function → (a) Heat. Heat depends on the route between states, not just the end states.
  5. (v) State function → (g) Internal energy, (k) Entropy, (l) Pressure. All three depend only on the state of the system, not on how it was reached.
  6. (vi) ΔU=q\Delta U = q → (b) At constant volume. At constant volume, w=0w = 0, so ΔU=qV\Delta U = q_V.
  7. (vii) Law of conservation of energy → (c) First law of thermodynamics. The First Law, ΔU=q+w\Delta U = q + w, is the energy-conservation statement.
  8. (viii) Reversible process → (j) Infinitely slow process which proceeds through a series of equilibrium states. A reversible (quasi-static) change passes through equilibrium states.
  9. (ix) Free expansion → (h) pext=0p_{\text{ext}} = 0. Expansion into a vacuum, so w=−pextΔV=0w = -p_{\text{ext}}\Delta V = 0.
  10. (x) ΔH=q\Delta H = q → (i) At constant pressure. At constant pressure, ΔH=qp\Delta H = q_p.
  11. (xi) Intensive property → (l) Pressure and (m) Specific heat. Both are independent of the amount of substance (specific heat is heat capacity per unit mass), so both are intensive.
  12. (xii) Extensive property → (g) Internal energy, (k) Entropy. Both scale with the amount of substance. …

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