Step 1: Identify the dimensions of the given physical quantities.
The dimensions of the length-scale l l l , permittivity ε \varepsilon ε , Boltzmann constant k B k_{\text{B}} k B , absolute temperature T T T , number density n n n , and charge q q q are determined from their physical definitions.
[ l ] = L [l] = L [ l ] = L
[ ε ] = [ q 2 ] [ F ] [ r 2 ] = M − 1 L − 3 T 4 I 2 [\varepsilon] = \frac{[q^2]}{[F][r^2]} = M^{-1}L^{-3}T^4 I^2 [ ε ] = [ F ] [ r 2 ] [ q 2 ] = M − 1 L − 3 T 4 I 2
[ k B ] = [ energy ] [ T ] = M L 2 T − 2 Θ − 1 [k_{\text{B}}] = \frac{[\text{energy}]}{[T]} = ML^2 T^{-2} \Theta^{-1} [ k B ] = [ T ] [ energy ] = M L 2 T − 2 Θ − 1
[ T ] = Θ [T] = \Theta [ T ] = Θ
[ n ] = L − 3 [n] = L^{-3} [ n ] = L − 3
[ q ] = I T [q] = IT [ q ] = I T
Step 2: Find the dimensions of key combinations.
Determine the dimension of the combination ε k B T \varepsilon k_{\text{B}} T ε k B T .
[ ε k B T ] = ( M − 1 L − 3 T 4 I 2 ) ( M L 2 T − 2 Θ − 1 ) ( Θ ) [\varepsilon k_{\text{B}} T] = (M^{-1}L^{-3}T^4 I^2)(ML^2 T^{-2} \Theta^{-1})(\Theta) [ ε k B T ] = ( M − 1 L − 3 T 4 I 2 ) ( M L 2 T − 2 Θ − 1 ) ( Θ )
[ ε k B T ] = L − 1 T 2 I 2 [\varepsilon k_{\text{B}} T] = L^{-1}T^2 I^2 [ ε k B T ] = L − 1 T 2 I 2
Determine the dimension of the combination q 2 ε k B T \dfrac{q^2}{\varepsilon k_{\text{B}} T} ε k B T q 2 .
[ q 2 ε k B T ] = I 2 T 2 L − 1 T 2 I 2 \left[\frac{q^2}{\varepsilon k_{\text{B}} T}\right] = \frac{I^2 T^2}{L^{-1}T^2 I^2} [ ε k B T q 2 ] = L − 1 T 2 I 2 I 2 T 2
[ q 2 ε k B T ] = L \left[\frac{q^2}{\varepsilon k_{\text{B}} T}\right] = L [ ε k B T q 2 ] = L
Step 3: Test the dimensional correctness of Option 1.
Check the dimension of the expression n q 2 ε k B T \sqrt{\dfrac{nq^{2}}{\varepsilon k_{\text{B}} T}} ε k B T n q 2 .
[ n q 2 ε k B T ] = [ n ] ⋅ [ q 2 ε k B T ] \left[\sqrt{\frac{nq^{2}}{\varepsilon k_{\text{B}} T}}\right] = \sqrt{[n] \cdot \left[\frac{q^2}{\varepsilon k_{\text{B}} T}\right]} ε k B T n q 2 = [ n ] ⋅ [ ε k B T q 2 ]
[ n q 2 ε k B T ] = L − 3 ⋅ L \left[\sqrt{\frac{nq^{2}}{\varepsilon k_{\text{B}} T}}\right] = \sqrt{L^{-3} \cdot L} ε k B T n q 2 = L − 3 ⋅ L
[ n q 2 ε k B T ] = L − 1 ≠ L \left[\sqrt{\frac{nq^{2}}{\varepsilon k_{\text{B}} T}}\right] = L^{-1} \neq L ε k B T n q 2 = L − 1 = L
Step 4: Test the dimensional correctness of Option 2.
Check the dimension of the expression ε k B T n q 2 \sqrt{\dfrac{\varepsilon k_{\text{B}} T}{nq^{2}}} n q 2 ε k B T .
[ ε k B T n q 2 ] = 1 [ n ] ⋅ [ ε k B T q 2 ] \left[\sqrt{\frac{\varepsilon k_{\text{B}} T}{nq^{2}}}\right] = \sqrt{\frac{1}{[n]} \cdot \left[\frac{\varepsilon k_{\text{B}} T}{q^2}\right]} [ n q 2 ε k B T ] = [ n ] 1 ⋅ [ q 2 ε k B T ]
[ ε k B T n q 2 ] = L 3 ⋅ L − 1 \left[\sqrt{\frac{\varepsilon k_{\text{B}} T}{nq^{2}}}\right] = \sqrt{L^3 \cdot L^{-1}} [ n q 2 ε k B T ] = L 3 ⋅ L − 1
[ ε k B T n q 2 ] = L \left[\sqrt{\frac{\varepsilon k_{\text{B}} T}{nq^{2}}}\right] = L [ n q 2 ε k B T ] = L
Step 5: Test the dimensional correctness of Option 3.
Check the dimension of the expression q 2 ε n 2 / 3 k B T \sqrt{\dfrac{q^{2}}{\varepsilon n^{2/3} k_{\text{B}} T}} ε n 2/3 k B T q 2 .
[ q 2 ε n 2 / 3 k B T ] = [ n − 2 / 3 ] ⋅ [ q 2 ε k B T ] \left[\sqrt{\frac{q^{2}}{\varepsilon n^{2/3} k_{\text{B}} T}}\right] = \sqrt{[n^{-2/3}] \cdot \left[\frac{q^2}{\varepsilon k_{\text{B}} T}\right]} ε n 2/3 k B T q 2 = [ n − 2/3 ] ⋅ [ ε k B T q 2 ]
[ q 2 ε n 2 / 3 k B T ] = L 2 ⋅ L \left[\sqrt{\frac{q^{2}}{\varepsilon n^{2/3} k_{\text{B}} T}}\right] = \sqrt{L^2 \cdot L} ε n 2/3 k B T q 2 = L 2 ⋅ L
[ q 2 ε n 2 / 3 k B T ] = L 3 / 2 ≠ L \left[\sqrt{\frac{q^{2}}{\varepsilon n^{2/3} k_{\text{B}} T}}\right] = L^{3/2} \neq L ε n 2/3 k B T q 2 = L 3/2 = L
Step 6: Test the dimensional correctness of Option 4.
Check the dimension of the expression q 2 ε n 1 / 3 k B T \sqrt{\dfrac{q^{2}}{\varepsilon n^{1/3} k_{\text{B}} T}} ε n 1/3 k B T q 2 .
[ q 2 ε n 1 / 3 k B T ] = [ n − 1 / 3 ] ⋅ [ q 2 ε k B T ] \left[\sqrt{\frac{q^{2}}{\varepsilon n^{1/3} k_{\text{B}} T}}\right] = \sqrt{[n^{-1/3}] \cdot \left[\frac{q^2}{\varepsilon k_{\text{B}} T}\right]} ε n 1/3 k B T q 2 = [ n − 1/3 ] ⋅ [ ε k B T q 2 ]
[ q 2 ε n 1 / 3 k B T ] = L ⋅ L \left[\sqrt{\frac{q^{2}}{\varepsilon n^{1/3} k_{\text{B}} T}}\right] = \sqrt{L \cdot L} ε n 1/3 k B T q 2 = L ⋅ L
[ q 2 ε n 1 / 3 k B T ] = L \left[\sqrt{\frac{q^{2}}{\varepsilon n^{1/3} k_{\text{B}} T}}\right] = L ε n 1/3 k B T q 2 = L
Answer:
The dimensionally correct expressions are (2) ε k B T n q 2 \sqrt{\dfrac{\varepsilon k_{\text{B}} T}{nq^{2}}} n q 2 ε k B T and (4) q 2 ε n 1 / 3 k B T \sqrt{\dfrac{q^{2}}{\varepsilon n^{1/3} k_{\text{B}} T}} ε n 1/3 k B T q 2 .