Flag Thermal Physics> A composite bar of length L= L 1 + L 2 is...
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A composite bar of length L= L1 + L2 is made from a bar of material 1 and length L1 attached to a bar of material 2 and length L2 as shown in Fig. 21- 15. (a) show that effective coefficient of linear expansion α for this bar is given by α = (α1L1 + α2L2)/L, (b) using steel and brass, design such a composite bar whose length is 52.4 cm and whose effective coefficient of linear expansion is 13 ×10-6/C°
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

Shane Macguire , 10 Years ago
Grade upto college level
anser 1 Answers
Askiitians Tutor Team

To tackle the problem of finding the effective coefficient of linear expansion for a composite bar made of two different materials, we can break it down into two parts as you've outlined. Let's dive into each part step by step.

Understanding the Effective Coefficient of Linear Expansion

When two materials are joined together, each material expands differently when subjected to temperature changes. The effective coefficient of linear expansion (α) for the composite bar can be derived from the individual coefficients of linear expansion of the materials involved.

Part (a): Deriving the Effective Coefficient of Linear Expansion

Let’s denote:

  • α1: Coefficient of linear expansion for material 1
  • α2: Coefficient of linear expansion for material 2
  • L1: Length of material 1
  • L2: Length of material 2
  • L: Total length of the composite bar (L = L1 + L2)

When the temperature changes by ΔT, the change in length for each material can be expressed as:

  • ΔL1 = α1 * L1 * ΔT
  • ΔL2 = α2 * L2 * ΔT

The total change in length (ΔL) of the composite bar is the sum of the changes in length of both materials:

ΔL = ΔL1 + ΔL2 = α1 * L1 * ΔT + α2 * L2 * ΔT

Factoring out ΔT, we get:

ΔL = (α1 * L1 + α2 * L2) * ΔT

The effective coefficient of linear expansion (α) for the composite bar is defined as:

α = ΔL / (L * ΔT)

Substituting our expression for ΔL, we have:

α = (α1 * L1 + α2 * L2) / L

This shows that the effective coefficient of linear expansion for the composite bar is indeed given by:

α = (α1 L1 + α2 L2) / (L1 + L2)

Part (b): Designing a Composite Bar with Specific Properties

Now, let’s design a composite bar made of steel and brass that has a total length of 52.4 cm and an effective coefficient of linear expansion of 13 × 10-6 /°C.

We know the coefficients of linear expansion for the materials:

  • αsteel ≈ 11 × 10-6 /°C
  • αbrass ≈ 19 × 10-6 /°C

Let L1 be the length of the steel part and L2 be the length of the brass part. We can express the total length as:

L1 + L2 = 52.4 cm

Substituting into the effective coefficient formula:

13 × 10-6 = (11 × 10-6 * L1 + 19 × 10-6 * L2) / 52.4

Multiplying both sides by 52.4 gives:

13 × 10-6 * 52.4 = 11 × 10-6 * L1 + 19 × 10-6 * L2

Calculating the left side:

13 × 10-6 * 52.4 = 0.000682

Now we have:

0.000682 = 11 × 10-6 * L1 + 19 × 10-6 * L2

We can express L2 as:

L2 = 52.4 - L1

Substituting this into the equation gives:

0.000682 = 11 × 10-6 * L1 + 19 × 10-6 * (52.4 - L1)

Expanding and rearranging leads to:

0.000682 = 11 × 10-6 * L1 + 0.0009996 - 19 × 10-6 * L1

0.000682 - 0.0009996 = (11 - 19) × 10-6 * L1

-0.0003176 = -8 × 10-6 * L1

Solving for L1 gives:

L1 = 39.7 cm

Substituting back to find L2:

L2

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