1. Use two convex lens instead of single lens.
2.

The magnification produced by the compound microscope
m = \(\frac{size\,of\,the\,image}{size\,of\,the\,object}\)
i.e, m = \(\frac{I_2M_2}{OB}\)
Multiplying and dividing by I1M1 we get,
m = \(\frac{I_2M_2}{I_1M_1}\times\frac{I_1M_1}{OB}\)
but we know, me = \(\frac{I_2M_2}{I_1M_1}\)and mo = \(\frac{I_1M_1}{OB}\)
Where m0 & me are the magnifying power of objective lens and eyepiece lens.
∴ m = me × m0 .......(1)
Eyepiece acts as a simple microscope.
Therefore me = 1 + \(\frac{D}{f_e}\) .....(2)
We know magnification of objective lens
m0 = \(\frac{V_0}{u_0}\) .....(3)
Where v0 and u0 are the distance of the image and object from the objective lens.
Substituting (2) and (3) in (1), we get
m = \(\frac{-V_0}{u_0}\Big(1+\frac{D}{f_e}\Big)\)
for compound microscope, u0 » f0 (because the object of is placed very close to the principal focus of the objective) and v0 ≈ L, length of microscope (because the first image is formed very close to the eye piece).
m = \(\frac{-L}{f_0}\Big(1+\frac{D}{f_e}\Big)\)
where L is the length of microscope, f0 is the focal length of objective lens.
3. Strain for eye, will be minimum when image is at infinity.