1) We can use the equation for linear thermal expansion:
ΔL = αLΔT
where ΔL is the change in length, α is the coefficient of linear thermal expansion, L is the original length, and ΔT is the change in temperature.
Let's assume that both bars expand by the same amount, so that the initial gap of 1.1 cm is exactly closed. We can set up an equation:
ΔL(steel) + ΔL(copper) = 1.1 cm
Using the equation above and the given coefficients of linear thermal expansion and original lengths, we can write:
α(steel)L(steel)ΔT + α(copper)L(copper)ΔT = 1.1 cm
Solving for ΔT, we get:
ΔT = 1.1 cm / (α(steel)L(steel) + α(copper)L(copper))
ΔT = 1.1 cm / (13 x 10^-6 K^-1 × 18.0 m + 16.5 x 10^-6 K^-1 × 10.0 m)
ΔT ≈ 139.9 K
Therefore, the change in temperature is approximately 139.9 K.
2) We can now use the equation for linear thermal expansion again to calculate the distances that the steel stretches:
ΔL(steel) = α(steel)L(steel)ΔT
ΔL(steel) = 13 x 10^-6 K^-1 × 18.0 m × 139.9 K
ΔL(steel) ≈ 0.0408 m
Therefore, the steel stretches by approximately 0.0408 m.
3) Similarly, we can calculate the distances that the copper stretches:
ΔL(copper) = α(copper)L(copper)ΔT
ΔL(copper) = 16.5 x 10^-6 K^-1 × 10.0 m × 139.9 K
ΔL(copper) ≈ 0.0230 m
Therefore, the copper stretches by approximately 0.0230 m.