Step 1: We know the relationships:
\[
\alpha = \frac{I_C}{I_E}, \quad \beta = \frac{I_C}{I_B}.
\]
Step 2: The total current is conserved in the transistor, so:
\[
I_E = I_C + I_B.
\]
Step 3: From the definition of \( \alpha \), we can express \( I_C \) as:
\[
I_C = \alpha I_E.
\]
Substituting this into the equation for \( \beta \):
\[
\beta = \frac{\alpha I_E}{I_B}.
\]
Step 4: Since \( I_E = I_B + I_C \), we can express \( I_B \) in terms of \( I_E \) and \( \alpha \):
\[
I_B = \frac{I_E}{1 - \alpha}.
\]
Step 5: Substituting this into the expression for \( \beta \), we get:
\[
\beta = \frac{\alpha}{1 - \alpha}.
\]