Skip to main content

Torque to rotate truncated cone

Short answer

Using element at axial distance z, radius r = z tanα, shear stress τ = μ ω r / t. Integrate torque: T = (π μ ω tan³α)/(2 t cosα) (z₂⁴ − z₁⁴). With ω = 10.472 rad/s, μ = 0.2 Pa·s, α = 30°, z₁=0.04 m, z₂=0.10 m, T = 0.356 N·m.

Oil of viscosity μ\mu = 2 poise fills the small gap of thickness 0.2 mm. Determine the torque required to rotate the truncated cone at constant speed of 100 rpm. Neglect fluid stress exerted on the circular bottom. [Figure: inverted truncated cone with 60° apex angle, rotating with angular velocity ω\omega in a conical casing; dimensions 40 mm and 60 mm marked on the height]

Reading of the figure: the cone has a full apex angle of 60∘60^\circ (half-angle α=30∘\alpha=30^\circ). The wetted frustum extends from 40 mm to 100 mm measured along the axis from the (imaginary) apex: 40 mm from the apex to the small end, and a frustum height of 60 mm. The gap measured normal to the surface is t=0.2t=0.2 mm.

Data: μ=2\mu=2 poise =0.2=0.2 Pa·s, N=100N=100 rpm, so ω=2π×10060=10.472\omega=\dfrac{2\pi\times100}{60}=10.472 rad/s.

    \____________/   large end, z2 = 100 mm from apex
     \          /
      \        /     frustum height z2 - z1 = 60 mm
       \______/      small end, z1 = 40 mm from apex
        \    /
         \  /
          \/  apex (imaginary), 60 deg
    oil gap t = 0.2 mm between cone and casing

Take an element at axial distance zz from the apex:

  • radius r=ztan⁡αr=z\tan\alpha
  • slant length ds=dzcos⁡αds=\dfrac{dz}{\cos\alpha}
  • shear stress τ=μωrt\tau=\mu\dfrac{\omega r}{t}
dT=τ (2πr ds) r=2πμωt r3cos⁡α dzdT=\tau\,(2\pi r\,ds)\,r=\frac{2\pi\mu\omega}{t}\,\frac{r^{3}}{\cos\alpha}\,dz T=2πμωtan⁡3αtcos⁡α∫z1z2z3dz=πμωtan⁡3α2 tcos⁡α(z24−z14)T=\frac{2\pi\mu\omega\tan^{3}\alpha}{t\cos\alpha}\int_{z_1}^{z_2}z^{3}dz=\frac{\pi\mu\omega\tan^{3}\alpha}{2\,t\cos\alpha}\left(z_2^{4}-z_1^{4}\right)

Substituting (tan⁡30∘=0.5774\tan30^\circ=0.5774, cos⁡30∘=0.8660\cos30^\circ=0.8660, z1=0.04z_1=0.04 m, z2=0.10z_2=0.10 m):

T=π(0.2)(10.472)(0.5774)32(0.0002)(0.8660)(0.104−0.044)=0.356 N⋅mT=\frac{\pi(0.2)(10.472)(0.5774)^{3}}{2(0.0002)(0.8660)}\left(0.10^{4}-0.04^{4}\right)=0.356\ \text{N·m}

Answer: T≈0.356 N⋅mT\approx0.356\ \text{N·m}. (If the figure dimensions differ, use the same formula with the correct z1z_1 and z2z_2.)

✓ Answer checked by Claude Opus 5.5 (high effort)

All Fluid Mechanics chapter 1 questions →