Consider a water tank shown in the figure. It has one wall at x = L and can be taken to be very wide in the z direction. When filled with a liquid of surface tension S and density ρ, the liquid surface makes angle θ₀ (θ₀ << 1) with the x-axis at x = L. If y(x) is the height of the surface then the equation for y(x) is:
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(take θ(x) = sin θ(x) = tan θ(x) =\(\frac{dy}{dx}, \) g is the acceleration due to gravity)
 

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  1. \(\frac{d^2 y}{dx^2} = \frac{\rho g}{S} x \)
  2. \(\frac{d^2 y}{dx^2} = \frac{\rho g}{S} y \)
  3. \(\frac{d^2 y}{dx^2} = \sqrt{\frac{\rho g}{S}}\)
  4. \(\frac{dy}{dx} = \sqrt{\frac{\rho g}{S}} x\)

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Option 2 : \(\frac{d^2 y}{dx^2} = \frac{\rho g}{S} y \)
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Correct option is: (2) d2y/dx2 = (ρg / S) y

Explanation:

Screenshot 2025-05-15 164242

Curvature = 1 / ROC = |d2y/dx2| / (1 + (dy/dx)2)3/2 ≈ |d2y/dx2| / (1 + 0)3/2 = d2y/dx2

(dy/dx) ≈ tan θ ≈ 0 (small angle approximation)

Change in pressure, ΔP = S × curvature

ΔP = S × d2y/dx2

Also, ΔP = ρgy

⇒ ρgy = S × d2y/dx2

⇒ d2y/dx2 = (ρg / S) y

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