1
AIEEE 2012
MCQ (Single Correct Answer)
+4
-1
A wooden wheel of radius $$R$$ is made of two semicircular part (see figure). The two parts are held together by a ring made of a metal strip of cross sectional area $$S$$ and length $$L.$$ $$L$$ is slightly less than $$2\pi R.$$ To fit the ring on the wheel, it is heated so that its temperature rises by $$\Delta T$$ and it just steps over the wheel. As it cools down to surrounding temperature, it process the semicircular parts together. If the coefficient of linear expansion of the metal is $$\alpha $$, and its Young's modulus is $$Y,$$ the force that one part of the wheel applies on the other part is : AIEEE 2012 Physics - Heat and Thermodynamics Question 433 English
A
$$2\pi SY\alpha \Delta T$$
B
$$SY\alpha \Delta T$$
C
$$\pi SY\alpha \Delta T$$
D
$$2SY\alpha \Delta T$$
2
AIEEE 2012
MCQ (Single Correct Answer)
+4
-1
Helium gas goes through a cycle $$ABCD$$ (consisting of two isochoric and isobaric lines) as shown in figure efficiency of this cycle is nearly : (Assume the gas to be close to ideal gas) AIEEE 2012 Physics - Heat and Thermodynamics Question 432 English
A
$$15.4\% $$
B
$$9.1\% $$
C
$$10.5\% $$
D
$$12.5\% $$
3
AIEEE 2012
MCQ (Single Correct Answer)
+4
-1
Out of Syllabus
A Carnot engine, whose efficiency is $$40\% $$, takes in heat from a source maintained at a temperature of $$500$$ $$K.$$ It is desired to have an engine of efficiency $$60\% .$$ Then, the intake temperature for the same exhaust (sink) temperature must be :
A
efficiency of Carnot engine cannot be made larger than $$50\% $$
B
$$1200$$ $$K$$
C
$$750$$ $$K$$
D
$$600$$ $$K$$
4
AIEEE 2011
MCQ (Single Correct Answer)
+4
-1
A thermally insulated vessel contains an ideal gas of molecular mass $$M$$ and ratio of specific heats $$\gamma .$$ It is moving with speed $$v$$ and it's suddenly brought to rest. Assuming no heat is lost to the surroundings, Its temperature increases by:
A
$${{\left( {\gamma - 1} \right)} \over {2\gamma R}}M{v^2}K$$
B
$${{\gamma {M^2}v} \over {2R}}K$$
C
$${{\left( {\gamma - 1} \right)} \over {2R}}M{v^2}K$$
D
$${{\left( {\gamma - 1} \right)} \over {2\left( {\gamma + 1} \right)R}}M{v^2}K$$

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