Let y1 = (1/x)sin x
Then ln y1 = ln[(1/x)sin x] = sinx*ln(1/x) = sinx*(-lnx) = -lnx/cscx
In the next step I use L'Hopital's Rule, since we have an indeterminate form of [infinity/infinity]. Also, in the following steps, lim means limit as x -->0+
lim ln[ ln y1] = lim [-lnx/cscx]
= lim [(-1/x)/(-csc x * cot x)] = lim[(1/x)/(csc x * cot x)]
= lim[(1/x)/(1/sinx * cos x/sinx)] = lim [sin^2(x)/(x cos x)]
= lim [(sin(x)/x * tan(x)] = lim[sin(x)/x]*lim tan(x) = 1*0 = 0.
Since lim ln y1 = 0, ln lim y1 = 0, hence lim y1 = 1.
The other limit is easier.
Let y2 = sinx1/x = (eln(sinx))1/x = e(1/x)ln(sin x)
Before taking the limit, let's look at what the factors in the exponent on e are doing as x --> 0+.
1/x --> + infinity.
sin(x) --> 0+, so ln(sin(x)) --> -infinity.
The product of 1/x and ln(sin(x)) --> -infinity.
Since the exponent on e is approaching -infinity, then e to that power --> 0.
Hence lim y2 = lim e(1/x)ln(sin x) = 0.
Therefore lim (y1 + y2) = 1 + 0 = 1.