The amount of work done to break a big water drop of radius 'R' into 27 small drops of equal radius is 10 J. The work done required to break the same big drop into 64 small drops of equal radius will be :-
A.15 J
B.10 J
C.20 J
D.5 J
Solution & Explanation
Related Formula
The work done W$W$ in expanding surface area with surface tension S$S$ is given by:
W = S · Δ A$$W = S \cdot \Delta A$$
Core Logic
By volume conservation during splitting :
(4)/(3)π R³ = n ((4)/(3)π r³) r = Rn1/3$$\frac{4}{3}\pi R^{3} = n \left(\frac{4}{3}\pi r^{3}\right) \implies r = \frac{R}{n^{1/3}}$$
Work scales scaling-wise linearly with the key multiplier index (n1/3 - 1)$(n^{1/3} - 1)$. Taking ratios between targets directly avoids calculations of constants.
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
More Mechanical Properties of Fluids Previous-Year Questions — Page 3
A vessel with square cross-section and height of 6~m$6\mathrm{~m}$ is vertically partitioned. A small window of 100~cm²$100\mathrm{~cm}^2$ with hinged door is fitted at a depth of 3~m$3\mathrm{~m}$ in the partition wall. One part of the vessel is filled completely with water and the other side is filled with the liquid having density 1.5× 10³~kg/m³$1.5\times 10^{3}\mathrm{~kg/m}^{3}$. What force one needs to apply on the hinged door so that it does not get opened? (Acceleration due to gravity = 10~m/s²$= 10\mathrm{~m/s}^2$)
Numerical Answer.Answer: 150 to 150
Solution
Related Formula
P = P₀ + ρ g h$$P = P_0 + \rho g h$$F = Δ P · A$$F = \Delta P \cdot A$$
Core Logic
Let's analyze the pressure acting on the window at depth h = 3~m$h = 3\mathrm{~m}$ from both sides:
Water side (density ρw = 1.0 × 10³~kg/m³$\rho_w = 1.0 \times 10^3\mathrm{~kg/m}^3$):
The window has area A = 100~cm² = 100 × 10⁻⁴~m² = 10⁻²~m²$A = 100\mathrm{~cm}^2 = 100 \times 10^{-4}\mathrm{~m}^2 = 10^{-2}\mathrm{~m}^2$.
To keep the door from opening, we must apply a force balancing the pressure difference:
F = Δ P · A = 15000 × 10⁻² = 150~N$$F = \Delta P \cdot A = 15000 \times 10^{-2} = 150\mathrm{~N}$$
Step 1: Final Conclusion
The required force is
$
Step 1: Final Conclusion
The required force is $
150\mathrm{~N}.
Pattern Recognition
For a vertical interface between two fluids, the net pressure difference is simply given by
$.
Pattern Recognition
For a vertical interface between two fluids, the net pressure difference is simply given by $
\Delta P = \Delta \rho \cdot g h. The ambient atmospheric pressure$. The ambient atmospheric pressure $P_0$ cancels out since it acts on both sides of the window.
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
Qjee_main_2025_03_april_eveningWork Done by Gravity in Connecting Vessels
Two cylindrical vessels of equal cross sectional area of 2~m²$2\mathrm{~m}^{2}$ contain water upto height 10~m$10\mathrm{~m}$ and 6~m$6\mathrm{~m}$, respectively. If the vessels are connected at their bottom then the work done by the force of gravity is :
(Density of water is 10³~kg/m³$10^{3}\mathrm{~kg/m}^{3}$ and g=10~m/s²$g=10\mathrm{~m/s}^{2}$)
A.1 × 10⁵~J$1 \times 10^{5}\mathrm{~J}$
B.4 × 10⁴~J$4 \times 10^{4}\mathrm{~J}$
C.6 × 10⁴~J$6 \times 10^{4}\mathrm{~J}$
D.8 × 10⁴~J$8 \times 10^{4}\mathrm{~J}$
Solution
Related Formula
The gravitational potential energy U$U$ of a liquid column of mass m$m$ and height h$h$ is evaluated relative to its bottom by placing its total mass at its center of mass (h/2$h/2$):
U = m g ((h)/(2)) = (ρ A h) g ((h)/(2)) = (1)/(2) ρ A g h²$$U = m g \left(\frac{h}{2}\right) = (\rho A h) g \left(\frac{h}{2}\right) = \frac{1}{2} \rho A g h^2$$
Work done by the force of gravity (W$W$) equals the negative change in potential energy:
W = -Δ U = Uᵢ - Uf$$W = -\Delta U = U_i - U_f$$
Core Logic
Since the vessels are identical and connected at the bottom, water flows from the higher column to the lower one until their final heights equalize at:
Step 1: Calculate Initial Potential Energy (Uᵢ$U_i$)
Let the reference level U=0$U=0$ be at the bottom:
Uᵢ = U₁ + U₂ = (1)/(2) ρ A g h₁² + (1)/(2) ρ A g h₂²$$U_i = U_1 + U_2 = \frac{1}{2} \rho A g h_1^2 + \frac{1}{2} \rho A g h_2^2$$Uᵢ = (1)/(2) ρ A g (10² + 6²) = (1)/(2) ρ A g (100 + 36) = 68 ρ A g$$U_i = \frac{1}{2} \rho A g \left(10^2 + 6^2\right) = \frac{1}{2} \rho A g (100 + 36) = 68 \rho A g$$
Work Done by Gravity in Connecting Vessels
Step 2: Calculate Final Potential Energy (Uf$U_f$)
Both vessels equalize to hf = 8~m$h_f = 8\mathrm{~m}$:
Uf = 2 × [ (1)/(2) ρ A g hf² ] = ρ A g (8²) = 64 ρ A g$$U_f = 2 \times \left[ \frac{1}{2} \rho A g h_f^2 \right] = \rho A g (8^2) = 64 \rho A g$$
Step 3: Work Done by Gravity (W$W$)
W = Uᵢ - Uf = 68 ρ A g - 64 ρ A g = 4 ρ A g$$W = U_i - U_f = 68 \rho A g - 64 \rho A g = 4 \rho A g$$
Substitute the given values (ho = 10³~kg/m³$
ho = 10^3\mathrm{~kg/m}^3$, A = 2~m²$A = 2\mathrm{~m}^2$, g = 10~m/s²$g = 10\mathrm{~m/s}^2$):
For leveling liquids between two identical connected columns, the shift in center of mass always simplifies. The loss in potential energy is given by
$
Pattern Recognition
For leveling liquids between two identical connected columns, the shift in center of mass always simplifies. The loss in potential energy is given by $
\Delta U = \frac{1}{4} \rho A g (h_1 - h_2)^2. Applying this directly:$. Applying this directly:
$Δ U = (1)/(4) × 10³ × 2 × 10 × (10 - 6)² = 5000 × 16 = 8 × 10⁴~J$\Delta U = \frac{1}{4} \times 10^3 \times 2 \times 10 \times (10 - 6)^2 = 5000 \times 16 = 8 \times 10^4\mathrm{~J}$$
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
Q12jee_main_2025_03_april_eveningViscosity and Terminal Velocity
A solid steel ball of diameter 3.6~mm$3.6\mathrm{~mm}$ acquired terminal velocity 2.45×10⁻²~m/s$2.45\times10^{-2}\mathrm{~m/s}$ while falling under gravity through an oil of density 925~kg~m⁻³$925\mathrm{~kg~m}^{-3}$. Take density of steel as 7825~kg~m⁻³$7825\mathrm{~kg~m}^{-3}$ and g as 9.8~m/s²$9.8\mathrm{~m/s}^{2}$. The viscosity of the oil in SI unit is :
A. 2.18
B. 2.38
C. 1.68
D. 1.99
Solution
Related Formula
Terminal velocity vₜ$v_t$ of a spherical body falling through a viscous fluid is given by Stokes' Law:
vₜ = (2)/(9) r² g (ρbody - ρfluid)η$$v_t = \frac{2}{9} \frac{r^2 g (\rho_{\text{body}} - \rho_{\text{fluid}})}{\eta}$$
Hence, the viscosity coefficient η$\eta$ is:
η = (2)/(9) r² g (ρbody - ρfluid)vₜ$$\eta = \frac{2}{9} \frac{r^2 g (\rho_{\text{body}} - \rho_{\text{fluid}})}{v_t}$$
r = d/2$). Always ensure all numerical parameters are converted cleanly to SI base units (meters, kilograms, seconds) before applying Stokes' formula.
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
Q22jee_main_2025_03_april_eveningExcess Pressure in Soap Bubbles
The excess pressure inside a soap bubble A in air is half the excess pressure inside another soap bubble B in air. If the volume of the bubble A is n$n$ times the volume of the bubble B, then the value of n$n$ is ________.
Numerical Answer.Answer: 8 to 8
Solution
Related Formula
Excess pressure inside a soap bubble in air (which has two liquid-gas interfaces) is given by:
Δ P = (4T)/(R) ⇒ R ∝ (1)/(Δ P)$$\Delta P = \frac{4T}{R} \Rightarrow R \propto \frac{1}{\Delta P}$$
The volume V$V$ of a spherical bubble of radius R$R$ is:
V = (4)/(3)π R³ ⇒ V ∝ R³ ∝ ((1)/(Δ P))³$$V = \frac{4}{3}\pi R^3 \Rightarrow V \propto R^3 \propto \left(\frac{1}{\Delta P}\right)^3$$
VA = n VB ⇒ n = (VA)/(VB) = ((RA)/(RB))³ = (2)³ = 8$$V_A = n V_B \Rightarrow n = \frac{V_A}{V_B} = \left(\frac{R_A}{R_B}\right)^3 = (2)^3 = 8$$
Pattern Recognition
Volume scale factors depend on the cube of linear scale factors (V ∝ R³$V \propto R^3$). Since radius is inversely proportional to excess pressure, a halving of excess pressure leads to doubling of radius, scaling volume by 2³ = 8$2^3 = 8$.
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
Q22jee_main_2025_08_april_eveningBulk Modulus
A sample of a liquid is kept at 1~atm$1\mathrm{~atm}$. It is compressed to 5~atm$5\mathrm{~atm}$ which leads to change of volume of 0.8~cm³$0.8\mathrm{~cm}^{3}$. If the bulk modulus of the liquid is 2~GPa$2\mathrm{~GPa}$, the initial volume of the liquid was ________ litre. (Take 1~atm = 10⁵~Pa$1\mathrm{~atm} = 10^{5}\mathrm{~Pa}$)
Numerical Answer.Answer: 4 to 4
Solution
Related Formula
B = -(Δ P)/(Δ V / V) V = B (-Δ V)/(Δ P)$$B = -\frac{\Delta P}{\Delta V / V} \implies V = B \frac{-\Delta V}{\Delta P}$$
where,
B$B$ = Bulk modulus of liquid
Δ P$\Delta P$ = change in pressure
Δ V$\Delta V$ = change in volume
V$V$ = initial volume
Thus, the initial volume was 4~litres$4\mathrm{~litres}$.
Pattern Recognition
Sees: Bulk modulus definition calculation.
Trap: Watch out for unit conversions: 1~GPa = 10⁹~Pa$1\mathrm{~GPa} = 10^9\mathrm{~Pa}$, and 1~cm³ = 10⁻⁶~m³$1\mathrm{~cm}^3 = 10^{-6}\mathrm{~m}^3$. Finally, express the answer in Litres, where 1~L = 10⁻³~m³$1\mathrm{~L} = 10^{-3}\mathrm{~m}^3$. ✓
Chapter Mix
Class 11 Physics: Mechanical Properties of Fluids
More Mechanical Properties of Fluids Questions — jee_main_2025_24_jan_morning
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.