To solve this problem, we need to understand the principle of linear expansion of materials due to temperature changes. The coefficient of linear expansion, $\alpha$, represents how much a material expands per degree change in temperature. If the initial length of a rod is $l_0$ and the temperature changes by $\Delta T$, the change in length $\Delta l$ can be calculated by:
$$ \Delta l = \alpha \cdot l_0 \cdot \Delta T $$
Given:
The condition implies that even after expansion due to temperature changes, the difference in lengths should remain the same:
$$ (l_2 + \Delta l_2) - (l_1 + \Delta l_1) = l_2 - l_1 $$
Substituting the formulas for linear expansion, we have:
$$ (l_2 + \alpha_2 l_2 \Delta T) - (l_1 + \alpha_1 l_1 \Delta T) = l_2 - l_1 $$
Simplifying the equation:
$$ l_2 + \alpha_2 l_2 \Delta T - l_1 - \alpha_1 l_1 \Delta T = l_2 - l_1 $$
Cancelling $(l_2 - l_1)$ from both sides, we get:
$$ \alpha_2 l_2 \Delta T = \alpha_1 l_1 \Delta T $$
Further simplifying, we find:
$$ \alpha_1 l_1 = \alpha_2 l_2 $$
Therefore, the correct relation that holds true is:
$$ \alpha_1 l_1 = \alpha_2 l_2 $$
This equation ensures that the expansion is such that the difference in lengths remains constant.
A particle is moving in a straight line. The variation of position $ x $ as a function of time $ t $ is given as:
$ x = t^3 - 6t^2 + 20t + 15 $.
The velocity of the body when its acceleration becomes zero is: