| η = | ⎛ ⎝ | F | ⎞ ⎠ | ÷ | ⎛ ⎝ | Δvx | ⎞ ⎠ | or | η = | ⎛ ⎝ | F | ⎞ ⎠ | ÷ | ⎛ ⎝ | dvx | ⎞ ⎠ |
| A | Δz | A | dz |
| Catalog No. | Cup No. | Orifice, inch | Liquid type | Zahn range, seconds (250°C) | Range, Centistokes |
| 3410-01 | 1 | 0.078 | Very thin | 45-80 | 18-56 |
| 3401-02 | 2 | 0.108 | Thin | 25-80 | 40-230 |
| 3401-03 | 3 | 0.148 | Medium | 20-75 | 150-790 |
| 3401-04 | 4 | 0.168 | Heavy-thick | 20-80 | 220-1100 |
| 3401-05 | 5 | 0.208 | Very heavy-thick | 20-75 | 460-1725+ |
V= K (T – C)
where: V is Kinematic Viscosity (cSt)
T is Efflux time (Zahn seconds)
K + C are constants ( Ref. # 1)
SPECIFIC FORMULAS
Zahn cup # Formula “T range seconds”
1 V = 1.1 ( T-29) 45-80
2 V = 3.5 (T-14) 25-80
3 V= 11.7 (T-7.5) 20-75
4 V= 14.8 (T-5) 20-80
5 V= 23 (T-0) 20-75
What is drag?
Drag, in fluid dynamics, refers to forces that oppose the relative motion of an object through a fluid (a liquid or gas). Drag forces depend on velocity.
STOKE'S GREAT LAW OF DRAG
If
- r = the radius of a sphere in cm
d1 = the density of the sphere in g/cm3
d2 = the density of the fluid in g/cm3
g = the local gravitational acceleration in cm/S2
c = the Viscosity of the fluid in Poise
v = the terminal velocity in cm/S
Then
- From this, I can derive that the more viscous the fluid, the smaller the terminal velocity. Thus, I can form an hypothesis for my experiment (how does viscosity affect the movement of a pendulum in terms of speed?): The higher the viscosity of the liquid, the slower the pendulum will travel, therefore, the longer the time taken for one oscillation.
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