To solve this problem, we need to apply the principle of calorimetry, which states that the heat lost by the hot body is equal to the heat gained by the cooler bodies when there is no loss of heat to the surroundings.
Let's breakdown the problem:
Applying the formula:
\text{Heat lost by copper ball} = \text{Heat gained by calorimeter} + \text{Heat gained by water}
Mathematically,
m_1 c_\text{copper} (T - 75) = m_2 c_\text{copper} (75 - 30) + m_3 c_\text{water} (75 - 30)
Let's substitute the given values:
100 \times 0.1 \times (T - 75) = 100 \times 0.1 \times 45 + 170 \times 1 \times 45
This simplifies to:
10(T - 75) = 450 + 7650
10(T - 75) = 8100
Dividing both sides by 10:
T - 75 = 810
Adding 75 to both sides gives:
T = 885^{\circ} C
Therefore, the initial temperature $T$ of the copper ball is $885^{\circ} C$.
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: