282. Nusselt number (for forced convection heat transfer) is a function of the _________ number.
Prandtl
Reynolds
Both (A) & (B)
Neither (A) nor (B)
Correct answer: (C) Both (A) & (B)
283. Nusselt number is a function of Prandtl number and _________ number of fluid in natural convection heat transfer.
Grashoff
Biot
Stanton
Reynolds
Correct answer: (A) Grashoff
284. Nusselt number is the ratio of the
Temperature gradient of the wall to that across the entire pipe
Temperature difference to the temperature gradient at the wall
Heat flux at the wall to that across the entire pipe
None of these
Correct answer: (C) Heat flux at the wall to that across the entire pipe
285. Nusselt number is the ratio of the temperature gradient at the wall to
Temperature difference
Heat flux
That across the entire pipe
None of these
Correct answer: (C) That across the entire pipe
286. One kilogram of water at 0°C is changed to superheated steam of one atm pressure and 300° C. The major heat consumption in the process will be to
Heat the water from 0°C to 100°C
Evaporate the water
To superheat the steam
Data insufficient, can't be predicted
Correct answer: (B) Evaporate the water
287. Open pan evaporators are preferred to be used, when the solution to be concentrated is
Scaling
Highly viscous
Corrosive
Salty
Correct answer: (B) Highly viscous
288. Out of 100 kcal/second of incident radiant energy on the surface of a thermally transparent body, 300 kcal/second is reflected back. If the transmissivity of the body is 0.25, the emissivity of the surface will be
0.35
0.45
0.55
0.85
Correct answer: (B) 0.45
289. Out of the following four assumptions used in the derivation of the equation for LMTD [LMTD = (Δt1 - Δt2)/ln(Δt1/Δt2)], which one is subject to the largest deviation in practice ?
Constant overall heat transfer co-efficient.
Constant rate of fluid flow
Constant specific heat
No partial phase change in the system
Correct answer: (B) Constant rate of fluid flow
290. Overall heat transfer co-efficient for cooling of hydrocarbons by water is about