- #1
RobosaurusRex
- 29
- 1
Can someone show me how Faxen's 2nd law for the viscous torque on a rotating sphere comes to be?
I know tau_(r phi) = -3 mu Omega sin(theta)
Torque is integral of vec(r) cross vec(f)
But I can't get the right answer so I am doing something very wrong
Help?
I know tau_(r phi) = -3 mu Omega sin(theta)
Torque is integral of vec(r) cross vec(f)
But I can't get the right answer so I am doing something very wrong
Help?