05 Exercise Solutions - e
05 Exercise Solutions - e
During time t =5 to 10 s , Simon walks towards the 3. Take the upward direction as positive.
sensor at an average velocity of 0.2 m s−1. Given: u =5 m s−1 a =−9.81 m s−2 t =3 s
We can have to find s.
Slope = =0.2 m s−1
By the equation
2. Graphs:
= −29.145 m
Hence, the cliff is 29.145 m high.
Exercise
Checkpoint 7 (p.61)
1. Table:
time / s velocity / m s−1 displacement / m
0 20 0
1 10 15 Therefore, the smallest and the largest
2 0 20 displacements of the marble are 2 cm and 6 cm
3 −10 15 respectively.
4 −20 0 6. Electronic timing is more accurate than using
2. (a) F stopwatches.
Both balls accelerate at the same rate under It is because the finishing times of the swimmers
gravity, regardless of what they are made of. in competitions are very close. The error due to
(b) T the timekeeper’s reaction time would affect the
Its upward motion is slowing down. rankings if stopwatches were used.
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.3
= = 0.03611 h θ ≈ 63.4°
2= v = 20 m s-1
The speed of the boat is 20 m s−1 after 6 s.
Overall displacement: 5. Take the forward direction as positive. When the
s= = 223.6 km minibus speeds up, by , we have
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.5
3= t=5s 4. A
Graphs B and D mismatch the decelerating and
When it slows down, by , we have accelerating stages. Graph C fails in the final stage.
−1.5 = t =10 s Option B could be correct if the backward
The total time of travel =5+10+10= 25 s. direction of the bus was taken as positive. But it is
not natural. Besides, there are too many types of
6. (a) Take the forward direction as positive.
motion that can produce such an a–t graph.
By , we have
5. (a) Plot of the s–t graph:
a= = −0.6 m s-2
So the deceleration of the train is 0.6 m s−2.
(b) By , we have
−0.6 = t = 10 s
The train takes a further 10 s to stop.
7. Take the direction away from the racket as positive.
By , we have
a= = 32 m s-2
The acceleration of the ball is 32 m s−2 away from
the racket.
(b) Velocity = slope of the s–t graph
8. (a) The skater slides up the ramp with a
= = 0.04 m s-1
decreasing speed until she reaches the
highest point, where she is momentarily at The average velocity of the tank is 0.04 m s−1
rest. Then she slides down the ramp with an forward.
increasing speed. 6. (a) Take the forward direction as positive.
(b) Take the direction up the ramp as the Sketch of the v–t graph:
positive. By , we have
−0.8 = t=5s
She will reach a speed of 2 m s−1 again 5 s
later.
(c) Area = = 6300 m2 7. (a) From the graph, the shop is 160 m due east
of Jeff’s home.
2. A
(b) Velocity during time t = 0 to 5 min:
The s–t graph shows that the two cars have the
same displacement at t = T. v= = 0.533 m s-1
(c) The total distance travelled by Jeff (b) Let T be the required time. The following
= (160)(2) = 320 m. shows the s–t graph of Sara.
The total displacement of Jeff = 0.
8. (a) During t = 0 to 0.5 s, the acceleration = 3/0.5
= 6 m s−2 away from the sensor.
During t =0.5 to 2 s, the acceleration = 0.
(b) The trolley accelerates uniformly at 6 m s−2
away from the sensor during t = 0 to 0.5 s.
Then it travels at a constant velocity of
3 m s−1 away from the sensor during t = 0.5
to 2 s.
(c) The overall displacement of the trolley
Consider the slope of the s–t graph during
= t = 10 to T, we have
= 5.25 m away from the sensor. T = 15 s
9. (a) For time t = 0 to 35 s , the acceleration
(c) When she goes back, her velocity
= ≈ 0.571 m s−2.
For time t =35 to 100 s, the acceleration = 0.
= 4 m s−1.
For time t = 100 to 140 s, the acceleration
Therefore, the plot of the v–t graph becomes
= = −0.5 m s−2.
Therefore, the a–t graph is
3(2T − 2) = 4(2T − 4)
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.7
3T − 3 = 4T − 8 s
T=5s Let s1 be the displacement of the runner during
13. (a) The velocity of the car during t = 0 to 10 s the acceleration. By v2 − u2 = 2as, we have
= = 7 m s−1. 102 − 0 = 2(3.3)s or s1 =15.15 m.
The displacement of the runner after the
The velocity of the car during t = 20 to 30 s
acceleration is s2 = 100 − 15.15 = 84.85 m.
= = 1 m s−1.
Therefore, t2 = s2 / v2 = 84.85/10 = 8.485 s. The
First of all, the car starts moving from the
finishing time of the runner = 3.030 + 8.485
starting point at a constant speed of 7 m s−1
≈ 11.5 s.
during t = 0 to10 s. And then it decelerates
from v = 7 to 1 m s−1 during t = 10 to 20 s. It 7. (a) By , we have
finally moves at a constant speed of 1 m s−1 a = 3 m s-2
during t = 20 to 30 s.
The acceleration is 3 m s−2 forward.
(b) The average velocity
(b) At t =4 s, we have
= ≈ 3.67 m s−1 forward.
14. (a) The trolley in case A moves at a constant
velocity while that in case B accelerates. Therefore, x = 24.
(b) The trolley in case B has a higher average 8. (a) Take the direction to the left as positive.
velocity. The number of ticks on the tapes of At t = 2 s, we have
A and B are 9 and 7 respectively. The trolley
in case B takes less time to travel the same
distance, and hence it has a higher average (b) By v = u + at, we have
velocity. v = 0 + (6)(3) = 18 m s−1.
(c) The distance travelled by the deer during the
chase is s' = 27 − 18 = 9 m. So the speed of
Exercise 5.5 (p.50)
the deer v' = s'/t' = 9/3 = 3 m s−1.
1. A
9. (a) Take the direction to the left as positive.
Nancy measures the values of the time t and the
displacement s in order to find the acceleration a. 450 km h-1 = = 125 m s-1
Since we know that the initial velocity u = 0, the By v2 − u2 = 2as, we have
best option is A. v2 − 1252 = 2(−5)(1200)
2. B Therefore,
Given that u = 0. By v2 − u2 = 2as, we have v=
v2 − 0 = 2ad = 60.21 ≈ 60.2 m s-1
3. C So the speed of the plane is 60.2 m s−1 when
vavg = it goes beyond the runway.
(b) By v2 − u2 = 2as, we have
4. Take the forward direction as positive. 0 − 60.212 = 2a(250)
By , we have
a=
t = 0.064 s
= −7.25 m s-2
5. (a) Take the direction to the right as positive. By The deceleration of the plane is 7.25 m s−2
v = u + at, we have 1 = 0 + a(0.02) or after it goes beyond the runway.
a =50 m s−2. The acceleration of the ball is
(c) Let t1 and t2 be the time intervals that the
50 m s−2 towards the right.
plane moves on the runway and the field
(b) Yes. respectively. Since
The black ball will fall into the pocket v = u + at
because by v2 − u2 = 2as, we have
we have
02 − 0.42 = 2(−0.1) s or s =0.8 m > 0.7 m.
t1 = = 12.96 s
6. Take the forward direction as positive. Let t1 and t2
be the time taken for the runner to accelerate and t2 = = 8.305 s
move at a constant velocity respectively.
So the total time taken
By v = u + at, we have 10 = 0 + (3.3)t1 or t1 =3.030
= 12.96 + 8.305 ≈ 21.3 s.
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.8
10. (a) From the graph, his reaction time is 0.8 s. Exercise 5.6 (p.61)
1. D
(b) The acceleration = = −3.75 m s-2
The acceleration due to gravity always points
So the deceleration of the car is 3.75 m s−2. downwards regardless of the motion of the ball.
(c) Yes. 2. A
The car can stop before the traffic light. The graph given is a s–t graph, whose area under
The total distance travelled by the car the curve has no physical meaning.
= area under the v–t graph
3. C
= = 28.8 m < 32 m.
4. Take the downward direction as positive.
(d) No.
The car cannot stop before the traffic light.
The distance travelled by the car before
braking is s1 = v1 t1 = 15 × 0.8 =12 m. t = 4.778 s or −4.778 s (rejected)
By v2 − u2 = 2as, the distance travelled by the Average speed
car during the braking process is
0 − 152 = 2 (−3.75) s2 v= ≈ 23.4 m s-1
s2 = 30 m
Since the release takes place at t = 0, a negative
Hence, the total distance travelled by the car
time indicates a time instant before the release.
is 12 + 30 = 42 m > 40 m.
This solution is physically impossible and is
11. (a) Take the upstream direction as positive. therefore rejected.
Assume that the boat passes A at time t = 0.
5. (a) Take the downward direction as positive.
By , we have
Hence,
s1 = s= ≈ 5.87 m
the ball is at 5.87 m below the starting
s2 = point.
Combining the equations, we have 8. (a) Take the downward direction as positive.
s1 : s2 = −1200 : −400 = 3 : 1.
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.9
0 = 4.905t2 − 3t − 10
t = 1.766 ≈ 1.77 s or −1.154 s (rejected)
So she takes 1.77 s to reach the water
surface.
(b) v =u + at = −3+(9.81)(1.766) ≈ 14.3 m s−1
Her velocity when she reaches the water
surface is 14.3 m s−1 downward.
9. (a) Take the downward direction as positive.
By v = u + at , we have 0 = −2 + (9.81)(t) The area under the v–t graph is equal to the
⇒ t = 0.2039 s displacement of the object. So,
The fish reaches the highest point at t =
x= = 46.5 m
0.204 s.
(b) Consider the motion of the fish before it 3. C
reaches the highest point. Statement (1) is correct. At time t , the object is
momentarily at rest.
Statement (2) is incorrect. The acceleration of the
s= object at time t is determined by the slope of the
≈ −0.2039 m graph at that time, which takes a non-zero value.
Now consider the motion of the fish when it Statement (3) is incorrect. The displacement of
falls from the highest point to the table. the object at time t is determined by the area
under the graph during time = 0 to t, which takes a
non-zero value.
s= = 0.7697 m
4. D
So the total distance travelled by the fish Statement (1) is correct. The graphs have the same
= 0.2039 + 0.7697 = 0.9735 ≈ 0.974 m. slope when the cars are braking, and so they slow
The average speed of the fish down at the same rate.
= 0.9735/0.6 ≈ 1.62 m s−1. Statement (2) is incorrect. The reaction time of
(c) By v2 − u2 = 2as, we have the driver of car A is longer than that of car B .
v2 −22 = 2 (9.81)(0) Statement (3) is correct. As both cars have the
v2 = 4 same initial speed and slow down at the same rate,
v = 2 m s−1 or −2 m s−1 they travel the same distance when they
Since the downward direction is taken as decelerate.
positive, v < 0 represents an upward motion
5. C
and v >0 represents a downward motion. So
The acceleration of the ball is equal to the
the velocity is 2 m s−1 downward.
acceleration due to gravity g, which is constant
throughout the motion.
Chapter Exercise
6. A
Multiple-choice Questions (p.65)
If the object is thrown vertically downward, the
1. D time required to reach the bottom of the cliff
Statements (1) and (2) are correct as both cars decreases, but the acceleration (i.e. the slope of the
have the same displacement s at t =4 s. v–t graph) remains unchanged.
Statement (3) is correct. The s–t graphs of both 7. D
cars have increasing slopes throughout.
2. C
The slope of the graph is 2a. If a increases, the
From the v–t graph, the acceleration of the object
slope increases.
from t = 4 to 8 s is
8. C
a= = −3 m s-2
Statement (1) is possible. A car turning a corner at
By v = u + at, the velocity of the object at t = 5 s is a constant speed is accelerating.
v =12 + (−3)(1) = 9 m s−1. Statement (2) is possible. A ball being thrown
Therefore, we get upward is momentarily at rest (i.e. zero velocity)
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.10
at the highest point, but it is accelerating the shorter the time interval between which the
downwards. images are taken. So option A is the answer.
Statement (3) is impossible. Constant velocity Note that the equations of uniformly accelerated
implies constant speed and fixed direction of motion are independent of the mass of the object,
motion. so both options C and D are incorrect.
9. B 12. D
The speed of the ball during time t = 0 to 0.1 s is
u= = 0.36 m s-1
Therefore,
The speed of the ball during time t = 0.3 to 0.4 s is
v= = 0.2 m s-1
13. B
By v = u + at, we have
Statement (1) is incorrect. The sign of the velocity
0.2 = 0.36 + a (0.2) ⇒ a = −0.8 m s−2
of P does not change at t =1 s.
The deceleration of the ball is 0.8 m s−2.
Statement (2) is correct. At t = 2 s, the separation
10. C
between P and Q is
Assuming that the reaction time of the student is
negligible. The vertical height h and the time t' are sPQ = =4m
related by
Statement (3) is incorrect. At t = 4 s ,
sP = =2m
18 = u + 5a
Subtracting the equations, we have
18 − 9 = (u − u) + (5a − 2a) ⇒ a =3 m s−2.
T = 14.65 (1A)
time period is equal to the slope of the graph: reaction time t, in which g is the acceleration
due to gravity. (1A)
(b) No. (1A)
(1M)
Since ⇒ v2 =2gs, the slope (c) Any two of the following: (2A)
Find the height h fallen by the ruler. (1A) speed: scalar (1A)
Use the equation to find the
acceleration: scalar (1A)
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.12
(b) (i) (1) The velocity is represented by the (ii) Assume that car B catches up with car
slope of the graph. (1A) A at time t = 20 + T, which satisfies the
As the slope of the graph at t = 0 condition
is zero, the ball moves from rest. (vB − vA) × T = ∆s
(1A)
Using the result in (c)(i),
(2) The slope of the graph becomes (20 − 15) × T = 125 ⇒ T = 25 s (1M)
constant after t = 0.8 s. So air Car B catches up car A at
resistance cannot be neglected. t =20 + 25= 45 s. (1A)
(1A)
∴ t = 2.5 s
• Correct values: 1A The time required for the lorry to stop
• Correct lines: 1A completely is 2.5 s . As the collision happens
before the cars stop, we get T < 2.5 s. (1M)
(c) (i) The area under v–t graph of car A
Considering the displacement of the taxi and
tA = = 225 m
the lorry, we have
The area under v–t graph of car B
tB = = 100 m. (1M)
The separation between A and B
∆s =225 − 100= 125 m. (1A)
Considering the magnitude of the
displacements, we have
Active Physics Full Solutions to Textbook Exercises 05 Motion | p.13
30 = sT + (− sL)
∴ 30 = 20T − 4T2 + 15T − 4.5T2
0 = 8.5T2 − 35T + 30 (1M)
T = 1.217 ≈ 1.22 s or 2.90 s (rejected)
So the collision takes place at t = 1.22 s. (1A)
The displacement sL is negative.
(b) By , we have
s= ≈ 18.4 m
The position of the collision is 18.4 m away
from the position where the taxi applies the
brakes. (1A)