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# h2phy6 - Buoyant Force | # h2phym3- Hydraulic Lift - 3 |
# h2phy7 - Flow rate & Velocity | |
# h2phy8 - Surface Tension Force(1) | |
# h2phy9 - Volume & Mass Flow rate | |
# h2phy10 - Surface Tension Force(2) | ↰ |
(a) To what height will water (at 20 oC) rise in a glass tube
with a bore radius of 0.1 mm?
The contact angle for water in a glass tube is 0o
so the cos θ factor in figure 7, is equal to unity. Then,
(b) To what depth will mercury ( at 15oC) be
depressed in the same tube? In this case the contact
angle is 135o ; therefore,
(density of Mercury=13.6x103 kg.m-3)
Strategy - the rule "Must have" of Mr.Zhang ® |
|
→ | SI unit N.m-1 | |||
Ftension → (Forced required to stop movable side from sliding) | |||||
L(circumference ) =2πr ; because of the round shape of the surface. |
γ 2πr | = | FT | ||
We break down FT to FT (cosθ); | ||||
γ 2πr(cos θ) | = | FT (cosθ) | → (1) | Upward force ↑ |
mg | = | ρvg |
Table 8 Values of the Surface Tension for various liquids in contact with air | ||
Liquid | Temperature(oC) | -γ-(J/m2 or N/m) |
Acetone | 20 | 0.0237 |
Alcohol,methyl | 20 | 0.0226 |
Benzene | 20 | 0.0288 |
Water | 0 | 0.0756 |
Water | 20 | 0.0728 |
Water | 30 | 0.0712 |
Water | 100 | 0.0589 |
Mercury | 15 | 0.487 |
Solution |
(a) Compute to find the height by bringing equation (1)=(2) according to the equlibrium |
γ 2πr(cos θ) | = | (πr2h)(ρg) |
γ 2 | = | ( |
h | = |
2γcos θ
ρgr
|
h | = |
2(0.0728 N.m-1)
(103kg/m3)(9.8m/s2)(10-4m)
|
= | 0.15 m | |
Ans. Water (at 20 oC) rise 15 cm height in a glass tube. |
|
(b) To what depth will mercury ( at 15oC) be depressed in the same tube? In this case the contact angle is 135o ; therefore, (density of Mercury=13.6x103 kg.m-3) |
h | = |
2γcos135o
ρgr
|
h | = |
2(0.487 N.m-1)(-0.707)
(13.6x103 kg.m-3)(9.8 m.s-2(10-4 m)
|
h | = | -5.16 cm. |
Ans. Mercury (at 15 oC) will be depressed 5.16 cm. | ||
|
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