I've got data that, when plotted on a log-log scale, looks like two straight lines that gently bend and blend into each other. See the picture below.
I don't know how to find a function to fit that. Now, I know that I should use some kind of broken power law, and I know how to make one that asymptotically converges to a constant, but I don't know how to combine two power laws. I've found something that looks just right as far as its shape is concerned, and even some Python code to generate it, but I can't figure out how to tweak it to fit my data without breaking the continuity between the two power laws:
def chabrier03individual(m):
k = 0.158 * exp(-(-log(0.08))**2/(2 * 0.69**2))
return numpy.where(m <= 1,
0.158*(1./m) * exp(-(log(m)-log(0.08))**2/(2 * 0.69**2)), k*m**-2.3)
Note that here, log means $log_{10}$. Am I even on the right track?

What you provided in the previous question looked like a the cumulative data function (CDF), or survival function (SF), and this the probability density function (PDF). So this is a broken power law with a single break. You can either use the negative derivative of the SF from the previous question, which gives: \begin{align} f(x) & \equiv - N\frac{\partial B(x, s, \beta, x_n)}{\partial x} \\ & = - N\beta \left[1 + \left(\frac{x}{x_n}\right)^{|\beta|s}\right]^{\operatorname{sgn}(\beta)/s - 1} \left(\frac{x^{|\beta|s-1}}{x_n^{|\beta|s}}\right)^{|\beta|s}, \end{align} or, if you'd prefer to fit the pdf with its own smoothly broken power law that has a single break, you'd go for: $$ f(x) = N x^n \left[1+\left(\frac{x}{x_n}\right)^{|\beta|s}\right]^{\operatorname{sgn}(\beta)/s}, $$ which gives one more parameter than fitting the SF with a broken power law.