Q8. Two thin metallic spherical shells of radii π1 and π2π1 < π2 are placed with their centres coinciding. A material of thermal conductivity πΎ is filled in the space between the shells. The inner shell is maintained at temperature π1 and the outer shell at temperature π2π1 < π2 . The rate at which heat flows radially through the material is : (1) πΎπ2 - π1 (2) πΎπ2 - π1π2 - π1 π2 - π1 4ππ1π2 (3) ππΎπ1π2π2 - π1 (4) 4ππΎπ1π2π2 - π1 π2 - π1 π2 - π1
What This Question Tests
This question assesses the ability to derive or recall the formula for the rate of heat flow through a spherical shell, considering thermal conductivity and temperature difference.
Concepts Tested
Formulas Used
H = 4ΟK (T1 - T2) (r1r2 / (r2 - r1))
π NCERT Sections This Tests
2.4 β A Spherical Conductor Of Radius 12 Cm Has A Charge Of 1.6 Γ 10β7C
Physics Class 11 Β· Chapter 2
2.4 A spherical conductor of radius 12 cm has a charge of 1.6 Γ 10β7C distributed uniformly on its surface. What is the electric field (a) inside the sphere (b) just outside the sphere (c) at a point 18 cm from the centre of the sphere?
8.1 β Figure 8.5 Shows A Capacitor Made Of Two Circular Plates Each Of
Physics Class 11 Β· Chapter 8
8.1 Figure 8.5 shows a capacitor made of two circular plates each of radius 12 cm, and separated by 5.0 cm. The capacitor is being charged by an external source (not shown in the figure). The charging current is constant and equal to 0.15A. (a) Calculate the capacitance and the rate of change of potential difference between the plates. (b) Obtain the displacement current across the plates. (c) Is Kirchhoffβs first rule (junction rule) valid at each plate of the capacitor? Explain. FIGURE 8.5
11.3 β Zeroth Law Of Thermodynamics (A)
Physics Class 12 Β· Chapter 11
11.3 ZEROTH LAW OF THERMODYNAMICS (a) Imagine two systems A and B, separated by an adiabatic wall, while each is in contact with a third system C, via a conducting wall [Fig. 11.2(a)]. The states of the systems (i.e., their macroscopic variables) will change until both A and B come to thermal equilibrium with C. After this is achieved, suppose that the adiabatic wall between A and B is replaced by a conducting wall and C is insulated from A and B by an adiabatic wall [Fig.11.2(b)]. It is found that the states of A and B change no (b) further i.e. they are found to be in thermal Fig. 11.2 (a) Systems A and B are separated by an equilibrium with each other. This observation adiabatic wall, while each is in contact forms the basis of the Zeroth Law of with a third system C via a conducting Thermodynamics, which states that βtwo wall. (b) The adiabatic wall between A systems in thermal equilibrium with a third and B is replaced by a conducting wall, system separately are in thermal equilibrium while C is insulated from A and B by an adiabatic wall.with each otherβ. R.H. Fowler formulated this * Both the variables need not change. It depends on the constraints. For instance, if the gases are in containers of fixed volume, only the pressures of the gases would change to achieve thermal equilibrium. Reprint 2025-26 THERMODYNAMICS 229
π Question Details
- Chapter
- Thermodynamics & KTG
- Topic
- Heat transfer by conduction
- Year
- 2021
- Shift
- 31 Aug Shift 2
- Q Number
- Q8
- Type
- MCQ
- NCERT Ref
- Class 11 Physics Ch 11: Thermal Properties of Matter
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