To solve this problem, we can use the formula:
Q = mcΔT
where Q is the heat energy transferred, m is the mass of the water, c is the specific heat capacity of water (4.184 J/g°C), and ΔT is the change in temperature.
For the first part of the problem, we can use the formula to find the freezing point of the tap water:
Q1 = mcΔT1
where ΔT1 = 98°C - 60°C = 38°C
We assume that the mass of the water is the same in all experiments and in Dr. Woods' test, so we can use the same value of m throughout.
Q1 = mcΔT1 = m(4.184 J/g°C)(38°C)
Q1 = 1593.792 J
Each of the 3 other experiments raised the temperature of the water by 12.5°C, so the total change in temperature is:
ΔT2 = 12.5°C x 3 = 37.5°C
The heat energy transferred in these experiments is:
Q2 = mcΔT2 = m(4.184 J/g°C)(37.5°C)
Q2 = 1566.9 J
The total heat energy transferred before the water freezes is:
Q = Q1 + Q2 = 1593.792 J + 1566.9 J = 3160.692 J
We can now use the formula to find the freezing point of the tap water:
Q = mcΔTf
where ΔTf = T - 0°C
Assuming the same mass of water as before, we get:
3160.692 J = m(4.184 J/g°C)(60°C - 0°C)
m = 18.995 g
ΔTf = T - 0°C = 3160.692 J / (18.995 g x 4.184 J/g°C) ≈ 40°C
So, the freezing point of the tap water is approximately 40°C, which is 8 degrees higher than the normal freezing point of water (0°C).
For the second part of the problem, we can use the same formula to find the boiling point of the tap water:
Q = mcΔTb
where ΔTb = 100°C - T
Assuming the same mass of water as before, we get:
Q = mcΔTb = m(4.184 J/g°C)(99.25°C)
Q = 4158.83 J
4158.83 J = m(4.184 J/g°C)(T - 0°C)
T = 100°C + 4158.83 J / (18.995 g x 4.184 J/g°C) ≈ 116°C
So, the boiling point of the tap water is approximately 116°C, which is 16 degrees higher than the normal boiling point of water (100°C).