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JEE Advanced 2015 · Mechanical Properties of Fluids

A spherical body of radius RR consists of a fluid of constant density and is in equilibrium under its own gravity. If P(r)P(r) is the pressure at r (<R)r\,(<R), then the correct option(s) is (are)

Answers: B. P(r=3R/4)P(r=2R/3)=6380\frac{P(r=3R/4)}{P(r=2R/3)}=\frac{63}{80} · C. P(r=3R/5)P(r=2R/5)=1621\frac{P(r=3R/5)}{P(r=2R/5)}=\frac{16}{21}

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Written solution

Step 1: Find the gravitational field inside the sphere.

The mass enclosed within a radius rr (where r<Rr < R) for a constant density ρ\rho is given by the volume of the inner sphere.

M(r)=43πρr3M(r) = \frac{4}{3}\pi\rho r^{3}

The gravitational acceleration at radius rr depends only on this enclosed mass.

g(r)=GM(r)r2g(r) = \frac{GM(r)}{r^{2}} g(r)=43πGρrg(r) = \frac{4}{3}\pi G\rho r

Step 2: Set up the hydrostatic equilibrium equation.

The pressure gradient balances the inward gravitational force.

dPdr=−ρg(r)\frac{dP}{dr} = -\rho g(r)

Substitute the expression for g(r)g(r).

dPdr=−43πGρ2r\frac{dP}{dr} = -\frac{4}{3}\pi G\rho^{2} r

Step 3: Integrate to find the pressure profile P(r)P(r).

Integrate from radius rr to the surface RR, using the boundary condition that pressure at the surface is zero, P(R)=0P(R) = 0.

∫P(r)0dP=−∫rR43πGρ2r dr\int_{P(r)}^{0} dP = -\int_{r}^{R} \frac{4}{3}\pi G\rho^{2} r \, dr −P(r)=−23πGρ2(R2−r2)-P(r) = -\frac{2}{3}\pi G\rho^{2} (R^{2} - r^{2}) P(r)=23πGρ2(R2−r2)P(r) = \frac{2}{3}\pi G\rho^{2}(R^{2}-r^{2})

This can be written in terms of the central pressure Pc=P(0)P_c = P(0).

P(r)=Pc(1−r2R2)P(r) = P_c\left(1 - \frac{r^{2}}{R^{2}}\right) Pc=23πGρ2R2P_c = \frac{2}{3}\pi G\rho^{2}R^{2}

Step 4: Evaluate the pressure at the center.

Check the first option by evaluating the pressure at r=0r = 0.

P(0)=Pc≠0P(0) = P_c \neq 0

The pressure at the center is non-zero, so the first option is incorrect.

Step 5: Evaluate the ratio of pressures for the remaining options.

The ratio of pressures at any two distances aa and bb simplifies by canceling the constant factors.

P(a)P(b)=R2−a2R2−b2\frac{P(a)}{P(b)} = \frac{R^{2}-a^{2}}{R^{2}-b^{2}}

Test the ratio for a=3R4a = \frac{3R}{4} and b=2R3b = \frac{2R}{3}.

P(3R4)P(2R3)=1−9161−49\frac{P\left(\tfrac{3R}{4}\right)}{P\left(\tfrac{2R}{3}\right)} = \frac{1-\tfrac{9}{16}}{1-\tfrac{4}{9}} P(3R4)P(2R3)=71659\frac{P\left(\tfrac{3R}{4}\right)}{P\left(\tfrac{2R}{3}\right)} = \frac{\tfrac{7}{16}}{\tfrac{5}{9}} P(3R4)P(2R3)=6380\frac{P\left(\tfrac{3R}{4}\right)}{P\left(\tfrac{2R}{3}\right)} = \frac{63}{80}

Test the ratio for a=3R5a = \frac{3R}{5} and b=2R5b = \frac{2R}{5}.

P(3R5)P(2R5)=1−9251−425\frac{P\left(\tfrac{3R}{5}\right)}{P\left(\tfrac{2R}{5}\right)} = \frac{1-\tfrac{9}{25}}{1-\tfrac{4}{25}} P(3R5)P(2R5)=16252125\frac{P\left(\tfrac{3R}{5}\right)}{P\left(\tfrac{2R}{5}\right)} = \frac{\tfrac{16}{25}}{\tfrac{21}{25}} P(3R5)P(2R5)=1621\frac{P\left(\tfrac{3R}{5}\right)}{P\left(\tfrac{2R}{5}\right)} = \frac{16}{21}

Test the ratio for a=R2a = \frac{R}{2} and b=R3b = \frac{R}{3}.

P(R2)P(R3)=1−141−19\frac{P\left(\tfrac{R}{2}\right)}{P\left(\tfrac{R}{3}\right)} = \frac{1-\tfrac{1}{4}}{1-\tfrac{1}{9}} P(R2)P(R3)=3489\frac{P\left(\tfrac{R}{2}\right)}{P\left(\tfrac{R}{3}\right)} = \frac{\tfrac{3}{4}}{\tfrac{8}{9}} P(R2)P(R3)=2732≠2027\frac{P\left(\tfrac{R}{2}\right)}{P\left(\tfrac{R}{3}\right)} = \frac{27}{32} \neq \frac{20}{27}

Answer: The correct options are:

  • P(3R4)/P(2R3)=6380P\left(\frac{3R}{4}\right) / P\left(\frac{2R}{3}\right) = \frac{63}{80}
  • P(3R5)/P(2R5)=1621P\left(\frac{3R}{5}\right) / P\left(\frac{2R}{5}\right) = \frac{16}{21}

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