IB Mathematics SL 5.6 Derivatives of xn , sinx , cosx , tanx AA SL Paper 2- Exam Style Questions- New Syllabus
Sule Skerry and Rockall are small islands in the Atlantic Ocean, in the same time zone.
On a given day, the height of water in metres at Sule Skerry is modelled by the function \( H(t) = 1.63 \sin(0.513 \times (t – 8.20)) + 2.13 \), where \( t \) is the number of hours after midnight.
The following graph shows the height of the water for 15 hours, starting at midnight.
At low tide, the height of the water is 0.50 m. At high tide, the height of the water is 3.76 m. All heights are given correct to two decimal places.
On the same day, the height of water at Rockall is modelled by the function \( h(t) = a \sin(b \times (t – c)) + d \), where \( t \) is the number of hours after midnight, and \( a, b, c, d > 0 \).
The first low tide at Rockall occurs at 02:41, when the height is 0.40 m. The first high tide occurs at 09:02, when the height is 2.74 m.
a) The length of time between the first low tide and the first high tide is 6 hours and \( m \) minutes. Find the value of \( m \) to the nearest integer.
b) Between two consecutive high tides, determine the length of time, in hours, for which the height of the water is less than 1 metre.
c) Find the rate of change of the height of the water when \( t = 13 \), giving your answer in metres per hour.
d) Find the values of \( a, b, c, \) and \( d \).
e) When \( t = T \), the height of the water at Sule Skerry is the same as the height of the water at Rockall for the first time. Find the value of \( T \).
▶️ Answer/Explanation
a) To find the value of \( m \):
The water height at Sule Skerry is \( H(t) = 1.63 \sin(0.513 \times (t – 8.20)) + 2.13 \).
Period: \( \frac{2\pi}{0.513} \approx 12.238 \) hours.
Time from low to high tide is half the period:
\( \frac{12.238}{2} \approx 6.119 \) hours.
Convert to hours and minutes:
\( 6.119 – 6 = 0.119 \) hours.
\( 0.119 \times 60 \approx 7.14 \) minutes.
Rounding to the nearest integer:
\( m \approx 7 \) [3]
b) To find the time when the water height is less than 1 metre between consecutive high tides:
Solve \( H(t) < 1 \):
\( 1.63 \sin(0.513 \times (t – 8.20)) + 2.13 < 1 \)
\( 1.63 \sin(0.513 \times (t – 8.20)) < -1.13 \)
\( \sin(0.513 \times (t – 8.20)) < -\frac{1.13}{1.63} \approx -0.693 \)
Find boundary points where \( H(t) = 1 \):
\( \sin(0.513 \times (t – 8.20)) = -0.693 \)
Reference angle: \( \arcsin(0.693) \approx 0.766 \) radians.
Solutions in third and fourth quadrants:
\( 0.513 \times (t – 8.20) = \pi + 0.766 + 2k\pi \quad \text{or} \quad 2\pi – 0.766 + 2k\pi \)
\( = 3.908 + 2k\pi \quad \text{or} \quad 5.518 + 2k\pi \)
For one cycle starting at the first high tide (\( t \approx 11.261 \)) to the next (\( t \approx 23.499 \)):
For \( 0.513 \times (t – 8.20) = 3.908 \):
\( t – 8.20 = \frac{3.908}{0.513} \approx 7.616 \)
\( t \approx 8.20 + 7.616 = 15.816 \) hours.
For \( 0.513 \times (t – 8.20) = 5.518 \):
\( t – 8.20 = \frac{5.518}{0.513} \approx 10.756 \)
\( t \approx 8.20 + 10.756 = 18.956 \) hours.
Duration where \( H(t) < 1 \):
\( 18.956 – 15.816 \approx 3.14 \) hours.
Thus:
The length of time is approximately 3.14 hours [5]
c) To find the rate of change of water height at \( t = 13 \):
Compute the derivative:
\( H(t) = 1.63 \sin(0.513 \times (t – 8.20)) + 2.13 \)
\( H'(t) = 1.63 \times 0.513 \times \cos(0.513 \times (t – 8.20)) \approx 0.83619 \cos(0.513 \times (t – 8.20)) \)
Evaluate at \( t = 13 \):
\( H'(13) = 0.83619 \cos(0.513 \times (13 – 8.20)) \)
\( 13 – 8.20 = 4.80 \)
\( 0.513 \times 4.80 \approx 2.4624 \)
\( \cos(2.4624) \approx -0.778 \)
\( H'(13) \approx 0.83619 \times (-0.778) \approx -0.651 \)
Thus:
The rate of change is approximately \( -0.651 \) m/h [3]
d) To find the values of \( a, b, c, d \):
For Rockall: \( h(t) = a \sin(b \times (t – c)) + d \).
Given:
– Low tide at \( t = 2.6833 \) (02:41), height 0.40 m.
– High tide at \( t = 9.0333 \) (09:02), height 2.74 m.
Determine \( a \) and \( d \):
\( a = \frac{2.74 – 0.40}{2} = 1.17 \)
\( d = \frac{2.74 + 0.40}{2} = 1.57 \)
Low tide at \( t = 2.6833 \):
\( 0.40 = 1.17 \sin(b \times (2.6833 – c)) + 1.57 \)
\( 1.17 \sin(b \times (2.6833 – c)) = -1.17 \)
\( \sin(b \times (2.6833 – c)) = -1 \)
\( b \times (2.6833 – c) = -\frac{\pi}{2} + 2k\pi \quad (1) \)
High tide at \( t = 9.0333 \):
\( 2.74 = 1.17 \sin(b \times (9.0333 – c)) + 1.57 \)
\( 1.17 \sin(b \times (9.0333 – c)) = 1.17 \)
\( \sin(b \times (9.0333 – c)) = 1 \)
\( b \times (9.0333 – c) = \frac{\pi}{2} + 2m\pi \quad (2) \)
For first occurrences (\( k = 0 \), \( m = 0 \)):
\( b \times (2.6833 – c) = -\frac{\pi}{2} \quad (3) \)
\( b \times (9.0333 – c) = \frac{\pi}{2} \quad (4) \)
Subtract (3) from (4):
\( b \times (9.0333 – c – (2.6833 – c)) = \frac{\pi}{2} – \left(-\frac{\pi}{2}\right) \)
\( b \times 6.35 = \pi \)
\( b \approx \frac{\pi}{6.35} \approx 0.495 \)
Substitute \( b \approx 0.495 \) into (3):
\( 0.495 \times (2.6833 – c) = -\frac{\pi}{2} \approx -1.5708 \)
\( 2.6833 – c \approx \frac{-1.5708}{0.495} \approx -3.177 \)
\( c \approx 2.6833 + 3.177 \approx 5.860 \)
Thus:
\( a = 1.17 \), \( b \approx 0.495 \), \( c \approx 5.863 \), \( d = 1.57 \) [5]
e) To find \( T \) where \( H(T) = h(T) \):
\( 1.63 \sin(0.513 \times (T – 8.20)) + 2.13 = 1.17 \sin(0.495 \times (T – 5.863)) + 1.57 \)
Simplify:
\( 1.63 \sin(0.513 \times (T – 8.20)) – 1.17 \sin(0.495 \times (T – 5.863)) = -0.56 \)
Define:
\( f(T) = 1.63 \sin(0.513 \times (T – 8.20)) – 1.17 \sin(0.495 \times (T – 5.863)) + 0.56 \)
Solve \( f(T) = 0 \) numerically, testing around Rockall’s low tide (\( t = 2.6833 \)):
At \( T = 4.16 \):
\( H(4.16) \approx 1.63 \sin(0.513 \times (4.16 – 8.20)) + 2.13 \approx 0.60 \)
\( h(4.16) \approx 1.17 \sin(0.495 \times (4.16 – 5.863)) + 1.57 \approx 0.60 \)
Thus:
\( T \approx 4.16 \) [3]