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Grade 11IIT JEE Entrance Exam

A wooden wheel of radius R is made of two semi-circular parts (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 2pR. To fit the ring on the wheel, it is heated so that its temperature rises by DT and it just steps over the wheel. As it cools down to surrounding temperature, it presses the semicircular parts together. If the coefficient of linear expansion of the metal is a and its Young's modulus is Y, the force that one part of the wheel applies on the other part is

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Profile image of Abhishek Dogra
5 Years agoGrade 11
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ApprovedApproved Tutor Answer1 Year ago

To find the force that one part of the wooden wheel applies on the other part due to the contraction of the heated metal ring, we need to consider several factors, including the properties of the metal, the geometry of the ring, and the thermal expansion principles involved. Let’s break this down step by step.

Understanding Thermal Expansion

When materials are heated, they expand, and when they cool, they contract. The coefficient of linear expansion (α) quantifies how much a material expands per degree of temperature change. For our metal ring, if it is heated by a temperature change of ΔT, the change in length (ΔL) of the ring can be expressed as:

ΔL = α * L * ΔT

Applying the Concept to the Ring

Initially, the length of the metal ring is slightly less than the circumference of the wheel, which is 2πR. When heated, the ring expands and can fit over the wheel. Once it cools down, it contracts back to its original length, exerting a force on the wooden parts of the wheel.

Calculating the Change in Length

Let’s denote the original length of the ring as L. After heating, the new length becomes:

L' = L + ΔL = L + α * L * ΔT = L(1 + αΔT)

As the ring cools, it contracts back to its original length L, which creates a compressive force on the wooden parts of the wheel.

Force Exerted by the Metal Ring

The force exerted by the ring on the wooden parts can be derived from the relationship between stress, strain, and Young's modulus (Y). The stress (σ) in the ring when it cools can be defined as:

σ = Y * ε

Where ε (strain) is given by:

ε = ΔL / L

In our case, the change in length (ΔL) when the ring cools is equal to the original length L minus the contracted length L, which is:

ΔL = L - L(1 + αΔT) = -αLΔT

Substituting this into the strain equation gives:

ε = (-αLΔT) / L = -αΔT

Now, substituting ε into the stress equation:

σ = Y * (-αΔT)

Finding the Total Force

The total force (F) exerted by the ring can be calculated by multiplying the stress by the cross-sectional area (S) of the ring:

F = σ * S = (Y * (-αΔT)) * S

Thus, the force that one part of the wheel applies on the other part due to the contraction of the metal ring as it cools is:

F = -Y * αΔT * S

Summary of Key Points

  • The ring expands when heated and contracts when cooled.
  • The force exerted on the wooden parts of the wheel is due to the contraction of the ring.
  • The relationship between stress, strain, and Young's modulus allows us to calculate the force exerted.

This comprehensive approach highlights how thermal expansion and material properties interact to produce mechanical forces in structures. Understanding these principles is crucial in fields like engineering and materials science, where temperature changes can significantly impact the performance of components.