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Properties of Matter question

2010 · Shift 2 · Q40
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Properties of Matter question

2010 · Shift 2 · Q40

JEE AdvancedPhysicsProperties of MatterMCQ+3 / −0.75
When liquid medicine of density ρ\rhoρ is to be put in the eye, it is done with the help of a dropper. As the bulb on the top of the dropper is pressed, a drop forms at the opening of the dropper. We wish to estimate the size of the drop. We first assume that the drop formed at the opening is spherical because that requires a minimum increase in its surface energy. To determine the size, we calculate the net vertical force due to the surface tension T when the radius of the drop is R. When the force becomes smaller than the weight of the drop, the drop gets detached from the dropper. If the radius of the opening of the dropper is rrr, the vertical force due to the surface tension on the drop of radius R (assuming rrr << R) is
  1. A
    2πrT2\pi rT2πrT
  2. B
    2πRT2\pi RT2πRT
  3. C
    2πr2TR{{2\pi {r^2}T} \over R}R2πr2T​
  4. D
    2πR2Tr{{2\pi {R^2}T} \over r}r2πR2T​
View written solutionFree

Correct answer: C

  1. What force are we looking for?

    The liquid drop is attached to the circular opening of the dropper of radius rrr.

    Surface tension TTT acts tangentially along the contact line all around the rim.

    So, the total force due to surface tension is obtained by: F=T×(perimeter of contact)×(vertical component factor)F = T \times (\text{perimeter of contact}) \times (\text{vertical component factor})F=T×(perimeter of contact)×(vertical component factor)

  2. Perimeter of the contact line

    The contact line is the circular rim of the dropper opening, so its perimeter is 2πr2\pi r2πr

  3. Vertical component of surface tension

    Since the drop is spherical with radius RRR, and the opening radius is much smaller than the drop radius (r≪Rr \ll Rr≪R), the surface near the opening makes a small angle θ\thetaθ with the horizontal.

    From geometry of the sphere, sin⁡θ≈rR\sin\theta \approx \frac{r}{R}sinθ≈Rr​ for small rrr.

    The vertical component of surface tension per unit length is therefore Tsin⁡θ=TrRT\sin\theta = T\frac{r}{R}Tsinθ=TRr​

  4. Total vertical force

    Multiply by the full circumference: F=(2πr)(TrR)F = (2\pi r)\left(T\frac{r}{R}\right)F=(2πr)(TRr​)

    Hence, F=2πr2TRF = \frac{2\pi r^2 T}{R}F=R2πr2T​

  5. Matching with options

    This corresponds to: 2πr2TR\boxed{\frac{2\pi r^2 T}{R}}R2πr2T​​

    So the correct option is C.

  6. Comparison with stored answer

    Stored correct answer: C

    Our derived answer: C

    Therefore, they agree.

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