Statement 2: For two plates of equal thickness in contact (series) the equivalent thermal conductivity is given by 1/K=1/K_1 +1/K_2
Q184. Statement 1: A brass tumbler feels much colder than a wooden tray on a chilly day
Statement 2: The thermal conductivity of brass is less than that of wood
184 (c) The thermal conductivity of brass is high i.e., brass is a good conductor of heat. So, when a brass tumbler is touched, heat quickly flows from human body to tumbler. Consequently, the number appears colder, on the other hand wood is a bad conductor. So, heat does not flow from the human body to the wooden tray in this case. Thus it appears comparatively hotter
Statement 2: Wien’s displacement law states that T∝(1/λ_m)
185 (a) From Wien’s displacement law, temperature (T)∝1/λ_m (where λ_m is the maximum wavelength). Thus temperature of a body is inversely proportional to the wavelength. Since blue star has smaller wavelength and red star has maximum wavelength, therefore blue star is at higher temperature then red star
Statement 2: There is expansion of water below and above 4℃.
186 (a) Water has maximum density at 4℃. On heating above 4℃, density of water decreases and its volume increases. Therefore, water overflows in both the cases
Statement 2: Water has a high thermal conductivity
187 (b) During the day when water is cooler than the land, the wind blows off the water onto the land (as warm air rises and cooler air fills the place). Also at night, the effect is reversed (since the water is usually warmer than the surrounding air on land). Due to this wind flow the temperature near the sea coast remains moderate
Statement 2: Ice contracts on melting
188 (a) With rise in pressure melting point of ice decreases. Also ice contracts on melting
Statement 2: Air surrounding the fire conducts more heat upwards
189 (c) Heat is carried away from a fire sideways mainly by radiations. Above the fire, heat is carried by both radiation and by convection of air. The latter process carries much more heat
Statement 2: Heat transferred is directly proportional to the temperature gradient in each layer
190 (d) The correct reason is because under steady-state condition, when temperature becomes constant, the rate of conduction of heat across every lamina is the same