Q 1 :

When a block of iron floats in mercury at  0°C, fraction k1 of its volume is submerged, while at the temperature 60°C, a fraction k2 is seen to be submerged. If the coefficient of volume expansion of iron is γFe and that of mercury is γHg, then the ratio k1k2 can be expressed as                     [2001]

  • 1+60γFe1+60γHg

     

  • 1-60γFe1+60γHg

     

  • 1+60γFe1-60γHg

     

  • 1+60γHg1+60γFe

     

(1)

For equilibrium when temperature 0°C fig (a)

Upthrust=Wt. of body

∴   K1Vd2g=Vd1g

⇒  K1=d1d2             ⋯(i)

For equilibrium when temperature increases to 60° fig. (b)

When the temperature is increased the density will decrease.

∴  d1'=d1(1+γFe×60)

and   d2'=d2(1+γHg×60)

Again upthrust = Wt. of body

∴  K2V'd2'g=V'd1'g

∴  K2[d21+γHg×60]=d11+γFe×60

∴  K2[1+γFe×601+γHg×60]=d1d2

⇒  K1K2=1+γFe×601+γHg×60



Q 2 :

Steel wire of length 'L' at 40°C is suspended from the ceiling and then a mass 'm' is hung from its free end. The wire is cooled down from 40°C to 30°C to regain its original length 'L'. The coefficient of linear thermal expansion of the steel is 10-5/°C, Young's modulus of steel is 1011 N/m2 and radius of the wire is 1 mm. Assume that L≫diameter of the wire. Then the value of 'm' in kg is nearly               [2011]



(3)

We know that,  Y=F/AΔl/l

∴  Y=mg/AΔl/l=mglAΔl                ⋯(i)

Also, Δl=lαΔT                ⋯(ii)

From (i) and (ii)

Y=mglAlαΔT=mgAαΔT

∴  m=YAαΔTg=1011×π(10-3)2×10-5×1010=π≈3