In Fig. S2.9 oil of absolute viscosity\mu fills the small gap of thicknessY. (a) Neglecting fluid stress exerted on the circular underside, obtain an expression for the torqueT required to rotate the truncated cone at constant speed\omega. (b) What is the rate of heat generation, in joules per second, if the oil’s absolute viscosity is0.20 \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^2, \alpha=45^{\circ}, a=45 \mathrm{~mm}, b=60 \mathrm{~mm},Y=0.2 \mathrm{~mm}, and the speed of rotation is90 \mathrm{rpm} ?
(a) U=\omega r ; \quad for small gap Y, \frac{d u}{d y}=\frac{U}{Y}=\frac{\omega r}{Y}
Eq.(2.9) : \tau=\mu \frac{d u}{d y}=\frac{\mu \omega r}{Y} ; \quad d A=2 \pi r d s=\frac{2 \pi r d y}{\cos \alpha}
\begin{aligned} & \text { From Eq. (2.9): } \quad d F=\tau d A=\frac{\mu \omega r}{Y}\left(\frac{2 \pi r d y}{\cos \alpha}\right) \\\\ & d T=r d F=\frac{2 \pi \mu \omega}{Y \cos \alpha} r^3 d y ; \quad r=y \tan \alpha \\\\ & d T=\frac{2 \pi \mu \omega \tan ^3 \alpha}{Y \cos \alpha} y^3 d y \\\\ & T=\frac{2 \pi \mu \omega \tan ^3 \alpha}{Y \cos \alpha} \int_a^{a+b} y^3 d y ;\left.\quad \frac{y^4}{4}\right|_a ^{a+b}=\left[\frac{(a+b)^4}{4}-\frac{a^4}{4}\right] \\\\ & T=\frac{2 \pi \mu \omega \tan ^3 \alpha}{4 Y \cos \alpha}\left[(a+b)^4-a^4\right] \\\\ & \text { (b) }\left[(a+b)^4-a^4\right]=(0.105 \mathrm{~m})^4-(0.045 \mathrm{~m})^4=0.0001175 \mathrm{~m}^4 \\\\ & \omega=\left(90 \frac{\mathrm{rev}}{\mathrm{min}}\right)\left(2 \pi \frac{\text { radians }}{\mathrm{rev}}\right)\left(\frac{1 \mathrm{~min}}{60 \mathrm{~s}}\right)=3 \pi \mathrm{rad} / \mathrm{s}=3 \pi \mathrm{s}^{-1} \\\\ & \text { Heat generation rate }=\text { power }=T \omega=\frac{2 \pi \mu \omega^2 \tan ^3 \alpha}{4 Y \cos \alpha}\left[(a+b)^4-a^4\right] \\\\ & =\frac{2 \pi\left(0.20 \mathrm{~N} \cdot \mathrm{s} / \mathrm{m}^2\right)\left(3 \pi \mathrm{s}^{-1}\right)^2(1)^3\left[0.0001175 \mathrm{~m}^4\right]}{4\left(2 \times 10^{-4} \mathrm{~m}\right) \cos 45^{\circ}} \\\\ & =23.2 \mathrm{~N} \cdot \mathrm{m} / \mathrm{s}=23.2 \mathrm{~J} / \mathrm{s} \\\\ & \end{aligned}