You have a pole in the transfer function and an integrator, so to solve it if you are unsure split them up into two separate transfer functions and add the graphs.
First put the transfer function in familiar form:
[tex]G_{1}(s) = \frac{100}{(s+10)}[/tex]
and
[tex]G_{2}(s) = \frac{1}{s}[/tex]
For [tex]G_{1}(s)[/tex]
At low frequency the gain will be:
[tex]20log_{10}(100/10) = 20db[/tex]
At a value of around [tex]\omega = 10[/tex] The pole will kick in and produce an asymptote of -20db/decade.
For the integrator:
The integrator will have a value of 0db at [tex]\omega = 1[/tex] so if you start your graph at [tex]\omega = .01[/tex] it will start with a value of 40db and slope downwards at 20db per decade.
Adding both of those graphs gives a magnitude plot that starts at +60db (for omega = .01) and goes down -20db/decade until 10db, where it goes down -40db/decade for all omega.
This is a very simple transfer function, how were you taught these? Perhaps there is some fundamental misunderstanding.