Question #80974

A ball of radius 0.800mm and density 8.95gcm-3 is released from rest at the top of a tall glass tube filled with a liquid of coefficient of viscosity 0.60 Pas and density 0.900 gcm-3 .how long after release does the ball attain 98% of the terminal velocity?
1

Expert's answer

2018-09-17T15:13:09-0400

Answer on Question #80974, Physics / Other

A ball of radius 0.800mm and density 8.95gcm⁻³ is released from rest at the top of a tall glass tube filled with a liquid of coefficient of viscosity 0.60 Pas and density 0.900 gcm⁻³. how long after release does the ball attain 98% of the terminal velocity?

Solution:

Consider the movement of a ball inside a viscous fluid:

- Radius - r

- Coefficient of Viscosity - η

- Density of the ball - d

- Density of the liquid - ρ

- Acceleration due to Gravity - g

The ball is subjected to the influence of three forces: they are the weight, upthrust and the viscous force - drag or liquid friction.


Weight of the ball=mg=43πr3dg\text{Weight of the ball} = mg = \frac{4}{3} \pi r^3 dgUpthrust on the ball by the liquid=vρg=43πr3ρg\text{Upthrust on the ball by the liquid} = v \rho g = \frac{4}{3} \pi r^3 \rho g


According to Stokes Law,


Viscous force=6πηrV,\text{Viscous force} = 6 \pi \eta r V,


where V is the velocity at a given time.

At the outset, the downward force, weight, is greater than the combination of the upward forces. So, initially, the ball accelerates. The viscous force, which depends of the velocity, however, keeps increasing. As a result, at some point, the net force on the ball becomes zero and the velocity of the ball becomes constant.

It is the Terminal Velocity


Vt=2(dρ)gr29η=2×((8.950.90)×103kg/m3)×(9.8m/s2)×(0.8×103m)29×0.60Pas=0.0187m/sV_t = \frac{2(d - \rho) g r^2}{9 \eta} = \frac{2 \times ((8.95 - 0.90) \times 10^3 k g / m^3) \times (9.8 \, m / s^2) \times (0.8 \times 10^{-3} m)^2}{9 \times 0.60 \, \text{Pas}} = 0.0187 \, m / s


Set up the sum of forces:


ma=mgvρg6πηrVm a = m g - v \rho g - 6 \pi \eta r Va=(1ρd)g6πη43πr2dV=a = \left(1 - \frac{\rho}{d}\right) g - \frac{6 \pi \eta}{\frac{4}{3} \pi r^2 d} V ==(10.908.95)×9.86×0.6043×(0.8×103)2×8.95×103V=8.8145471.37V= \left(1 - \frac{0.90}{8.95}\right) \times 9.8 - \frac{6 \times 0.60}{\frac{4}{3} \times (0.8 \times 10^{-3})^2 \times 8.95 \times 10^3} V = 8.8145 - 471.37\,VdVdt=8.8145471.37V\frac{dV}{dt} = 8.8145 - 471.37\,V00.98VtdV8.8145471.37V=0tdt\int_{0}^{0.98V_t} \frac{dV}{8.8145 - 471.37\,V} = \int_{0}^{t} dt0.00212148log(8.8145471.37V)00.98Vt=t-0.00212148\, \log(8.8145 - 471.37\,V) \int_{0}^{0.98V_t} = t


So,


t=0.00212148log(8.8145471.37×0.98×0.0187)+0.00212148log(8.8145)=0.0083st = -0.00212148\, \log(8.8145 - 471.37 \times 0.98 \times 0.0187) + 0.00212148\, \log(8.8145) = 0.0083\,s


Answer: 0.0083 s

Answer provided by https://www.AssignmentExpert.com

Need a fast expert's response?

Submit order

and get a quick answer at the best price

for any assignment or question with DETAILED EXPLANATIONS!

Comments

No comments. Be the first!
LATEST TUTORIALS
APPROVED BY CLIENTS