A capillary tube of radius 0.1 mm is partly dipped in water (surface tension 70 dyn/cm and glass-water contact angle ≈ 0°) with 30° inclined with the vertical. The length of water risen in the capillary is:

❓ Question

A capillary tube of radius 0.1 mm is partly dipped in water (surface tension = 70 dyn/cm, contact angle ≈ ) with 30° inclination with the vertical. The length of water risen in the capillary is to be found.


🖼️ Question Image

A capillary tube of radius 0.1 mm is partly dipped in water (surface tension 70 dyn/cm and glass-water contact angle ≈ 0°) with 30° inclined with the vertical. The length of water risen in the capillary is:


✍️ Short Solution

Let’s recall the concept of capillary rise — the upward movement of liquid in a narrow tube due to surface tension.

For a vertical tube,

h=2Tcosθrρg​

But if the tube is inclined at an angle α with the vertical, then the actual length of the water column is longer than the vertical height:

l=hcosα​

🔹 Given Data

QuantitySymbolValue
Surface tensionTT
70 dyn/cm = 70 × 10⁻³ N/m
Radius of tuberr
0.1 mm = 1 × 10⁻⁴ m
Contact angleθ\theta
0° ⇒ cosθ = 1
Density of waterρ\rho
1000 kg/m³
Acceleration due to gravitygg
9.8 m/s²
Inclination angleα\alpha
30°

🧮 Step-by-Step Calculation

Step 1: Calculate vertical height hh

h=2Tcosθrρgh = \frac{2T \cos \theta}{r \rho g} h=2×70×103×1(1×104)×1000×9.8h = \frac{2 \times 70 \times 10^{-3} \times 1}{(1 \times 10^{-4}) \times 1000 \times 9.8} h=0.140.98=0.1429 m=14.29 cm

Step 2: Adjust for inclination

Since the tube is inclined at 30°,

l=hcos30°=14.290.866=16.5 cm

🧮 Image Solution

A capillary tube of radius 0.1 mm is partly dipped in water (surface tension 70 dyn/cm and glass-water contact angle ≈ 0°) with 30° inclined with the vertical. The length of water risen in the capillary is:

✅ Conclusion & Video Solution

Final Answer:

l=16.5cm​

📘 Concept Recap:

  • Capillary rise is caused by the balance of surface tension and weight of the liquid column.

  • Vertical rise (h) depends on surface tension, radius, and density.

  • When the tube is tilted, the water travels a longer path — hence l=h/cosαl = h / \cos α.

  • Smaller the radius, greater the rise!


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