Step 1: Understanding the setup.
Let the diverging lens be \( L_1 \) and the converging lens be \( L_2 \). The focal lengths of \( L_1 \) and \( L_2 \) are \( f_1 = -20 \, \text{cm} \) (diverging lens) and \( f_2 = +30 \, \text{cm} \) (converging lens). The distance between the two lenses is \( d = 15 \, \text{cm} \).
The object should be placed in such a way that the rays coming out of \( L_1 \) (diverging lens) and converging at \( L_2 \) form an image at infinity.
Step 2: Using the lens formula.
The lens formula for a single lens is given by:
\[
\frac{1}{f} = \frac{1}{v} - \frac{1}{u}
\]
where:
- \( f \) is the focal length of the lens,
- \( v \) is the image distance,
- \( u \) is the object distance.
For the diverging lens \( L_1 \), the image formed will be virtual, and the rays will diverge, but the image formed by \( L_1 \) will act as a virtual object for \( L_2 \).
Let the object distance for \( L_1 \) be \( u_1 \), and the image distance for \( L_1 \) be \( v_1 \). Then, the object distance for \( L_2 \) is:
\[
u_2 = d - v_1
\]
Now, applying the lens formula for \( L_1 \) and \( L_2 \), we can calculate \( u_1 \) to find the position where the object should be placed.
Step 3: Conclusion.
After solving the lens equations, the object should be placed at \( u_1 \approx 60 \, \text{cm} \) from the diverging lens \( L_1 \) so that the image is formed at infinity.