Where a=1, the curve looks like:

Increasing or decreasing the value of a will only change the radius of the curve.
To find when the curve begins and ends, set r=0, since this is where the curve is at the origin.
If asin3theta=0, then sin3theta=0. Since sintheta=0 at theta=0,pi,2pi... we see that for sin3theta, it will be 0 at 0,pi//3,2pi//3...
So, the curve in the first quadrant varies from theta=0 to theta=pi//3.
The expression for the area of any polar equation r from theta=alpha to theta=beta is given by 1/2int_alpha^betar^2d theta.
For one loop of the given equation, the corresponding integral is then 1/2int_0^(pi//3)(asin3theta)^2d theta.
Working this integral:
1/2int_0^(pi//3)(asin3theta)^2d theta=1/2int_0^(pi//3)a^2(sin^2 3theta)d theta
Use the identity cos2alpha=1-2sin^2alpha to rewrite for sin^2alpha, showing that sin^2alpha=1/2(1-cos2alpha).
We can use this to say that sin^2 3theta=1/2(1-cos6theta). Then the integral reduces:
=1/2int_0^(pi//3)a^2(1/2(1-cos6theta))d theta=a^2/4int_0^(pi//3)(1-cos6theta)d theta
Integrating term by term:
=a^2/4(theta-1/6sin6theta)|_0^(pi//3)
=a^2/4[pi/3-1/6sin2pi-(0-1/6sin0)]
=a^2/4(pi/3)
=(pia^2)/12