To determine the radius of curvature of the cooled strip, we can use the concept of thermal expansion and the fact that the length of the strip remains constant.
Let's denote the initial temperature of the strip as T1 and the final temperature after cooling as T2. The change in temperature is given as ΔT = T2 - T1.
First, let's calculate the change in length for each strip using the formula:
ΔL = α * L * ΔT
where ΔL is the change in length, α is the linear expansion coefficient, L is the original length of the strip, and ΔT is the change in temperature.
For the copper strip, α_copper = 1.70 * 10^-5 °C^(-1), L_copper = 29 mm, and ΔT = -5.1 K (negative because the temperature is reduced). Plugging in these values, we can calculate ΔL_copper:
ΔL_copper = (1.70 * 10^-5 °C^(-1)) * (29 mm) * (-5.1 K)
Similarly, for the steel strip, α_steel = 1.30 * 10^-5 °C^(-1) and ΔL_steel can be calculated using the formula above.
Next, let's determine the total change in length of the bimetallic strip by subtracting the change in length of the steel strip from the change in length of the copper strip:
ΔL_total = ΔL_copper - ΔL_steel
Now, the radius of curvature can be calculated using the formula:
1/R = (α_copper - α_steel) / d
where R is the radius of curvature and d is the difference in thickness between the two strips.
For this problem, the thickness of both strips is given as 1.1 mm.
Substituting the values for α_copper, α_steel, and d into the formula, we can solve for R.
Now, to determine the maximum deviation of the strip from the straight orientation, we can use the formula:
h = (R^2 - (d/2)^2)^(1/2) - (R - ((d/2)^2 + h^2)^(1/2))
Here, h represents the maximum deviation, R is the radius of curvature (calculated in part a), and d is the difference in thickness (given as 1.1 mm).
By rearranging the equation, we can solve for h.