Answer:
Explanation:
Part A:
Table for H(t) = −16t² + 90t + 50:
x y
1 124
2 166
3 176
4 154
Table for g(t) = 28 + 48.8t:
x y
1 76.8
2 125.6
3 174.4
4 223.2
H(t) = −16t² + 90t + 50
H(1) = −16(1)² + 90(1) + 50
H(1) = 124
H(t) = −16t² + 90t + 50
H(2) = −16(2)² + 90(2) + 50
H(2) = 166
H(t) = −16t² + 90t + 50
H(3) = −16(3)² + 90(3) + 50
H(3) = 176
H(t) = −16t² + 90t + 50
H(4) = −16(4)² + 90(4) + 50
H(4) = 154
g(t) = 28 + 48.8t
g(1) = 28 + 48.8(1)
g(1) = 76.8
g(t) = 28 + 48.8t
g(2) = 28 + 48.8(2)
g(2) = 125.6
g(t) = 28 + 48.8t
g(3) = 28 + 48.8(3)
g(3) = 174.4
g(t) = 28 + 48.8t
g(4) = 28 + 48.8(4)
g(4) = 223.2
The solution to H(t) = g(t) is located between the third and fourth second. The y values of H(t) and g(t) get closer and closer relative to the time, but at the fourth second the y values are farther apart. Between these two seconds, both tables of values would have the same ordered pair.
Part B:
The solution from part A for H(t) and g(t) represents the point where both objects pass while flying. At this point, the two objects would collide, changing their flight paths and equations. The equations of H(t) and g(t) are no longer valid after this point.