Concept:
Relation between collector current and base current is given by IC = βIB
Where, \({I_B} \propto A\;exp^\left( {\frac{{e{V_{BE}}}}{{KT}}} \right)\) also \( \frac{{{I_{{C_1}}}}}{{{I_{{C_2}}}}} = \frac{{{A_1}e^\left( {\frac{{e{V_{B{E_1}}}}}{{KT}}} \right)}}{{{A_2}e^\left( {\frac{{e{V_{B{E_2}}}}}{{KT}}} \right)}}\)
Application:
Assuming all other parameter is same for both of the BJT.
Now,
\( \frac{{{I_{{C_1}}}}}{{{I_{{C_2}}}}} = \frac{{{A_1}e^\left( {\frac{{e{V_{B{E_1}}}}}{{KT}}} \right)}}{{{A_2}e^\left( {\frac{{e{V_{B{E_2}}}}}{{KT}}} \right)}}\)
\(1 = \frac{{{{\left( {0.2 \times {{10}^{ - 6}}} \right)}^2}}}{{{{\left( {300 \times {{10}^{ - 6}}} \right)}^2}}}.e^\left[ {\frac{e}{{KT}}\left( {{V_{B{E_1}}} - {V_{B{E_2}}}} \right)} \right]\)
\(2.25 \times {10^6} = e^\left[ {\frac{{{V_{B{E_1}}} - {V_{B{E_2}}}}}{{{V_T}}}} \right]\)
\(ln\left( {2.25 \times {{10}^6}} \right) = \frac{{{V_{B{E_1}}} - {V_{B{E_2}}}}}{{{V_T}}}\)
\(14.626 \times {V_T} = {V_{B{E_1}}} - {V_{B{E_2}}}\)
\(\therefore{V_{B{E_1}}} - {V_{B{E_2}}} = 14.626 \times 26\;mV \)
= 380 mV