A metal metre scale that is accurate up to 0.5 mm is made at a temperature of 25$^\circ$C. The range of temperatures within which it can be used is (Coefficient of linear expansion of the metal = $10^{-5}$ /$^\circ$C)
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The formula for linear expansion, $\Delta L = \alpha L_0 \Delta T$, gives the change in length. When dealing with "accuracy" or "error", this implies using the absolute value of the change, $|\Delta L|$, as the scale can be either too long (at higher temperatures) or too short (at lower temperatures).
Step 1: Identify the given parameters.
The scale is a "metre scale", so its original length at the calibration temperature is $L_0 = 1$ m $= 1000$ mm.
The calibration temperature is $T_0 = 25^\circ$C.
The maximum allowed error in measurement is the change in length, $|\Delta L| \le 0.5$ mm.
The coefficient of linear expansion is $\alpha = 10^{-5}$ /$^\circ$C. Step 2: Use the formula for linear thermal expansion.
The change in length $\Delta L$ due to a change in temperature $\Delta T = T - T_0$ is given by:
\[
\Delta L = \alpha L_0 \Delta T.
\]
We are interested in the magnitude of the temperature change, so we use:
\[
|\Delta L| = \alpha L_0 |T - T_0|.
\] Step 3: Set up the inequality for the allowed temperature range.
We are given that the error must be at most 0.5 mm.
\[
\alpha L_0 |T - 25| \le 0.5.
\]
Substitute the given values:
\[
(10^{-5}) (1000) |T - 25| \le 0.5.
\]
\[
10^{-2} |T - 25| \le 0.5.
\] Step 4: Solve the inequality for T.
\[
|T - 25| \le \frac{0.5}{10^{-2}} = 0.5 \times 100 = 50.
\]
This inequality can be written as:
\[
-50 \le T - 25 \le 50.
\]
Add 25 to all parts of the inequality:
\[
-50 + 25 \le T \le 50 + 25.
\]
\[
-25 \le T \le 75.
\]
The range of temperatures is from -25$^\circ$C to +75$^\circ$C.