12th Grade > Physics
HEAT TRANSFER MCQs
Total Questions : 30
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Answer: Option A. -> 42.7∘ C
:
A
According to Newton law of cooling
θ1−θ2t=K[θ1−θ22−θ0]
For first process : (80−64)5=K[80+642−θ0] ....(i)
For second process : (80−52)10=K[80+522−θ0] ....(ii)
For third process : (80−θ)15=K[80+θ2−θ0] ....(iii)
On solving equation (i) and (ii) we get K=115 and θ0=24∘C . Putting these values in equation (iii) we get θ=42.7∘C
:
A
According to Newton law of cooling
θ1−θ2t=K[θ1−θ22−θ0]
For first process : (80−64)5=K[80+642−θ0] ....(i)
For second process : (80−52)10=K[80+522−θ0] ....(ii)
For third process : (80−θ)15=K[80+θ2−θ0] ....(iii)
On solving equation (i) and (ii) we get K=115 and θ0=24∘C . Putting these values in equation (iii) we get θ=42.7∘C
Question 22. The temperature of the two outer surfaces of a composite slab, consisting of two materials having coefficients of thermal conductivity K and 2K and thickness x and 4x, respectively are T2 and T1(T2>T1). The rate of heat transfer through the slab, in a steady state is (A(T2−T1)Kx)f , with f which equal to
Answer: Option D. -> 13
:
D
Equation of thermal conductivity of the given combination Keq=l1+l2l1K1+l2K2=x+4xxK+4x2K=53K . Hence rate of
flow of heat through the given combination is Qt=Keq.A(T2−T1))(x+4x)=53KA(T2−T1)5x=13KA(T2−T1)x
On comparing it with given equation we get f=13
:
D
Equation of thermal conductivity of the given combination Keq=l1+l2l1K1+l2K2=x+4xxK+4x2K=53K . Hence rate of
flow of heat through the given combination is Qt=Keq.A(T2−T1))(x+4x)=53KA(T2−T1)5x=13KA(T2−T1)x
On comparing it with given equation we get f=13
Question 23. Two conducting rods A and B of same length and cross-sectional area are connected (i) In series (ii) In parallel as shown. In both combination a temperature difference of 100∘ C is maintained. If thermal conductivity of A is 3K and that of B is K then the ratio of heat current flowing in parallel combination to that flowing in series combination is
Answer: Option A. -> 163
:
A
Heat current H=ΔθR⇒HpHs=RsRp
In first case : Rs=R1+R2=l(3K)A+lKA=43lKA
In second case : Rp=R1R2R1+R2=1(3K)A×lKA(l(3K)A+lKA)=l4KA
∴HpHs=4l3KAl4KA=163
:
A
Heat current H=ΔθR⇒HpHs=RsRp
In first case : Rs=R1+R2=l(3K)A+lKA=43lKA
In second case : Rp=R1R2R1+R2=1(3K)A×lKA(l(3K)A+lKA)=l4KA
∴HpHs=4l3KAl4KA=163
Answer: Option A. -> 0∘C
:
A
Suppose temperature difference between A and B is 100∘C and θA>θB
Heat current will flow from A to B via path ACB and ADB. Since all the rod are identical so Δθ)AC=(Δθ)AD
(Because heat current H=ΔθR ; here R = same for all.)
⇒θA−θC=θA−θD⇒θC=θD
i.e. temperature difference between C and D will be zero.
:
A
Suppose temperature difference between A and B is 100∘C and θA>θB
Heat current will flow from A to B via path ACB and ADB. Since all the rod are identical so Δθ)AC=(Δθ)AD
(Because heat current H=ΔθR ; here R = same for all.)
⇒θA−θC=θA−θD⇒θC=θD
i.e. temperature difference between C and D will be zero.
Answer: Option B. -> 780rρcσ
:
B
dTdt=σAmcJ(T4−T40) [In the given problem fall in temperature of body dT=(200-100)=100K , temp. of surrounding T0=0K, Initial temperature of body T=200k].
100dt=σ4πr243πr3ρcJ(2004−04)
⇒dt=rρcJ48σ×10−6s=rρcσ.4.248×10−6 [As J = 4.2]
780rρcσμs
:
B
dTdt=σAmcJ(T4−T40) [In the given problem fall in temperature of body dT=(200-100)=100K , temp. of surrounding T0=0K, Initial temperature of body T=200k].
100dt=σ4πr243πr3ρcJ(2004−04)
⇒dt=rρcJ48σ×10−6s=rρcσ.4.248×10−6 [As J = 4.2]
780rρcσμs
Question 26. An ice box used for keeping eatable cold has a total wall area of 1metre2 and a wall thickness of 5.0 cm. The thermal conductivity of the ice box is K=0.01joule/metre−∘C. It is filled with ice at 0∘ along with eatables on a day when the temperature is 30∘. The latent heat of fusion of ice is 334×103joules/kg . The amount of ice melted in one day is
(1 day =86,400 seconds )
(1 day =86,400 seconds )
Answer: Option D. -> 1552 gms
:
D
dQdt=KAldθ=0.01×10.05×30=6J/sec
Heat transferred in on day (86400 sec)
Q=6×86400=518400J
Now Q=mL⇒m=QL=518400334×103
=1.552kg=1552g.
:
D
dQdt=KAldθ=0.01×10.05×30=6J/sec
Heat transferred in on day (86400 sec)
Q=6×86400=518400J
Now Q=mL⇒m=QL=518400334×103
=1.552kg=1552g.
Answer: Option A. -> The level of alcohol in limb X falls while that in limb Y rises
:
A
Black bulb absorbs more heat in comparison with painted bulb. So air in black bulb expands more. Hence the level of alcohol in limb X falls while that in limb Y rises.
:
A
Black bulb absorbs more heat in comparison with painted bulb. So air in black bulb expands more. Hence the level of alcohol in limb X falls while that in limb Y rises.
Question 28. One end of a copper rod of uniform cross-section and of length 3.1 m is kept in contact with ice and the other end with water at 100∘ C. At what point along it's length should a temperature of 200∘ C be maintained so that in steady state, the mass of ice melting be equal to that of the steam produced in the same interval of time. Assume that the whole system is insulated from the surroundings. Latent heat of fusion of ice and vaporisation of water are 80 cal/gm and 540 cal/gm respectively
Answer: Option A. -> 21 cm from 100∘C end
:
A
Rate of flow of heat is given by dQdt=Δθl/KAalsodQdt=Ldmdt (where L = Latent heat)
⇒dmdt=KAl(ΔθL). Let the desire point is at a distance xfrom water at 100∘ C.
∵ Rate of ice melting = Rate at which steam is being produced
⇒(dmdt)Steam=(dmdt)Ice⇒(ΔθLl)Steam=(ΔθLl)Ice
⇒(200−100)540×x=(200−0)80(3.1−x)⇒x=0.21m=21cm
:
A
Rate of flow of heat is given by dQdt=Δθl/KAalsodQdt=Ldmdt (where L = Latent heat)
⇒dmdt=KAl(ΔθL). Let the desire point is at a distance xfrom water at 100∘ C.
∵ Rate of ice melting = Rate at which steam is being produced
⇒(dmdt)Steam=(dmdt)Ice⇒(ΔθLl)Steam=(ΔθLl)Ice
⇒(200−100)540×x=(200−0)80(3.1−x)⇒x=0.21m=21cm
Question 29. Four rods of identical cross-sectional area and made from the same metal form the sides of square. The temperature of two diagonally opposite points is T and √2 T respective in the steady state. Assuming that only heat conduction takes place, what will be the temperature difference between other two points
Answer: Option A. -> r1r2(r1−r2)
:
A
Consider a concentric spherical shell of radius r and thickness dr as shown in fig.
The radial rate of flow of heat through this shell in steady state will be H=dQdt=−KAdTdr=−K(4πr2)dTdr
⇒∫r2r1drr2=−4πKH∫T1T1dt
Which on integration and simplification gives
H=dQdt=4πKr1r2(T1−T2)r2−r1⇒dQdt∝r1r2(r2−r1)
:
A
Consider a concentric spherical shell of radius r and thickness dr as shown in fig.
The radial rate of flow of heat through this shell in steady state will be H=dQdt=−KAdTdr=−K(4πr2)dTdr
⇒∫r2r1drr2=−4πKH∫T1T1dt
Which on integration and simplification gives
H=dQdt=4πKr1r2(T1−T2)r2−r1⇒dQdt∝r1r2(r2−r1)