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Struggling with this question, please help with questions underlined or bracketed in yellow, help will be greatly appreciated!

From Acheson: Elementary Fluid Dynamics

7.2. A rigid sphere of radius a is immersed in an infinite expanse of viscous fluid. The sphere rotates with constant angular velocity Ω. The Reynolds number R-Ωα2/v is small, so that the slow flow equations apply (r, θ, φ) with θ=0 as the rotation axis, show that a purely rotary flow u us(r, θ)ee is possible provided that Using spherical polar coordinates (Ho sin θ)-0.

Write down the boundary conditions which иф must satisfy at and as r-oo, and hence seek an appropriate solution to eqn (7.72), thus finding r2 Show that the φ-component of stress on r-a is tφ -3μΩ sin θ, and deduce that the torque needed to maintain the rotation of the sphere is

Hint from the Book answer to the amount of torque needed at end of question:

7.2. u,-Ωr sin θ on r a. Try u,-/(r)sin θ. The torque exerted by the fluid on the sphere is

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    From Acheson: Elementary Fluid Dynamics Equation 7.3 and 6.12 (Slow Flow Equations) 7.2. A rigid sphere of radius a is immersed in an infinite expanse of viscous fluid. The sphere rotates with constant angular velocity Ω. The Reynolds number R-Ωα2/v is small, so that the slow flow equations apply (see eqns (7.3) and (6.12)). Using spherical polar coordinates (r, θ, φ) with θ-0 as the rotation axis, show that a purely rotary flow u us(r, e, s possible provided that...

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