I'm reading through Srednicki's QFT.
In Chapter 2, the author denotes an infinitesimal transformation by $$U(1+\delta \omega)=I+\frac{i}{2 \hbar}\delta \omega_{\mu \nu} M^{\mu \nu}.\tag{2.11}$$ Then using $U(\Lambda)^{-1}U(\Lambda')U(\Lambda)=U(\Lambda^{-1}\Lambda'\Lambda) \quad(\Lambda'=1+\delta \omega')$, the author gets $$\delta \omega_{\mu \nu}U(\Lambda)^{-1}M^{\mu \nu}U(\Lambda)=\delta \omega_{\mu \nu}\Lambda^\mu_{\ \ \rho}\Lambda^\nu_{\ \ \sigma}M^{\rho \sigma}.\tag{2.12}$$ But I don't quite understand how RHS goes to this form. I used $(\Lambda^{-1}M\Lambda)^{\mu \nu}=(\Lambda^{-1})^\mu_{\ \ \rho}M^{\rho\sigma}\Lambda_\sigma^{\ \ \nu}$ and $(\Lambda^{-1})^\mu_{\ \ \rho}=\Lambda_\rho^{\ \ \mu}$ for calculation, and I just can't get the right form in the textbook.
What's the right way to do the calculation?