nelson thornes answer to practice problems
DESCRIPTION
This PDF contains all the answers of the practice problems of the book "Mechanics and Radioactivity" by the Nelson Thornes Publication and it covers many different topics of Edexcel GCE and IAL physics syllabus.TRANSCRIPT
NAS Chemistry Teachers’ Guide © 2005 Nelson Thornes Ltd.
Section 6 –Solutions to Practice Questions
SN A
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 11 Length = (74.4 + 0.4) mm = 74.8 mm
Width = (32.7 + 0.4) mm = 33.1 mm
Height = (28.9 + 0.4) mm = 29.3 mm
2 Close micrometer and check for any zero error
Use it to measure combined thickness of all 56 pages (not the covers)
Page thickness = measurement/56 [≈ 5 mm/56 ≈ 0.09 mm]
3 E.g. the metre rule may have shrunk or its end may be 3 mm short
4 Percentage uncertainty = 0.05 mm × 100/(1.23 mm) = 4.1 %
5 Uncertainty = ± 4.7 kΩ × 2/100 = ± 94 Ω ≈ ± 100 Ω = ± 0.1 kΩPossible values range from 4.6 kΩ to 4.8 kΩ
Chapter 21 See experiment description on page 4
2 Mass = density × volume
(a) Volume of room = 4 m × 3 m × 2 m = 24 m3
Mass of air = 1.3 kg m–3 × 24 m3 = 31.2 kg = 31 kg
(b) Volume of Earth = 4πr3/3 = 4π × (6.35 × 106 m)3/3 = 8.04 × 1020 m3
Mass of Earth = 5500 kg m–3 × 8.04 × 1020 m3 = 4.42 × 1024 kg
(c) Volume of rod = πr2 × l = π × (0.2 cm)2 × 24 cm = 3.02 cm3
Mass of rod = 8.0 g cm–3 × 3.02 cm3 = 24 g
3 Volume = mass/density = 170 g/(2.7 g cm–3) = 63 cm3
Length3 = 63 cm3
Length of each side = 3.98 cm = 4.0 cm
4 Volume of cube = 5 cm × 5 cm × 5 cm = 125 cm3
Mass = density × volume = 2.5 g cm–3 × 125 cm3 = 313 g
5 Estimates: diameter = 10 cm; thickness = 1 mm; mass = 20 g
Volume of DVD = πr2 × t π × (5 cm)2 × 0.1 cm = 8 cm3
Density = mass/volume = 20 g/(8 cm3) = 2.5 g cm–3 = 2500 kg m–3
Similar to that of glass
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions6 Volume of mercury = mass/density = 10.1 g/(13.6 g cm–3) = 0.743 cm3
Volume of cylinder = πr2 × l = 0.743 cm3
r = √(0.743 cm3/(π × 10.5 cm)) = 0.150 cm
Internal diameter = 2r = 2 × 0.150 cm = 0.300 cm
Chapter 31 See Table 3.1 on page 7
2 Metre – the distance an electromagnetic wave travels in a vacuum in a time of 1/(299 792 458) s
Using this definition has the advantages that the metre can be reproduced anywhere in the worldand it does not vary with temperature like the original standard bar
A disadvantage is the difficulty imagining the distance travelled by such a fast wave in such a shorttime compared with observing the actual length of the original standard bar
3 A caesium atomic clock makes 9 192 631 770 oscillations every second
So in 1 day
Number of oscillations = 9 192 631 770 s–1 × 24 hour × 3600 s hour–1 = 794 243 384 928 000
4 Examples: 75 kg 32 mm 5.4 m s–1
75 kg = 75 × kg
5 13 Mm/(13 µm) = 13 × 106 m/(13 × 10–6 m) = 1 × 1012
Chapter 41 All quantities, other than base quantities, are called derived quantities
All derived quantities can be produced by suitable combinations of base quantities
2 Speed m s–1
Area m2
Volume m3
3 Density = mass/volume
Units are kg/m3 = kg m–3
4 Homogeneous means the same type
Can only equate or add together quantities which are of the same type
5 e.g. Density = 3 × mass/volume
Speed = distance/(4 × time)
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 51 Total distance = 3.5 km + 5.5 km = 9.0 km
Final displacement from home = 0 m
2 A scalar is a physical quantity where the magnitude is not associated with any particular direction …a scalar has only size while a vector has both size and direction
Scalars: distance, energy, volume, speed, mass
Vectors: acceleration, weight, displacement, velocity, force
3 Average speed = total distance travelled/total time taken
(a) Average speed = 100 m/(10 s) = 10 m s–1
(b) Average speed = 42 500 m/(2.25 hour × 3600 s hour–1) = 5.25 m s–1
4 Attach a measured length of card centrally to the trolley
Position the light gate so that the card blocks its beam as the trolley passes
Use an electronic timer to record the time interval for which the beam is blocked
Average speed = length of card/recorded time
5 Average speed = total distance travelled/total time taken
Both journeys are the same length L, so total distance is 2L
For each journey, time = distance/speed
Time to work = (L/3) seconds time to home = (L/9) seconds
Total time = (L/3) + (L/9) = (3L/9) + (L/9) = (4L/9) seconds
Average speed = 2L/(4L/9) = 2 × 9/4 = 4.5 m s–1
[OR chose a journey of, say, 90 m ]
[Time to work = 90 m/(3 m s–1) = 30 s ]
[Time to home = 90 m/(9 m s–1) = 10 s ]
[Total time = 30 s + 10 s = 40 s ]
[Average speed = 180 m/(40 s) = 4.5 m s–1 ]
Chapter 61 Average acceleration = change in velocity/time taken
a = (25.1 m s–1 – 3.4 m s–1)/(6.2 s) = 21.7 m s–1/(6.2 s) = 3.5 m s–2
2 Time taken = change in velocity/acceleration
t = (330 m s–1 – 75 m s–1)/(5 m s–2) = 255 m s–1/(5 m s–2) = 51 s
3 Attach a double interrupter card of measured ‘prong’ length x centrally to the trolley
Position the light gate so that the prongs block its beam as the trolley passes
Use an electronic timer to record:
the time intervals for which the beam is blocked t1 t2
the time interval between the interruptions t3
Average velocity = length of prong/recorded time
v1 = x/t1
v2 = x/t2
Acceleration a = (v1 – v2)/t3
4 ‘rate of ’ means ‘divided by time’
so ‘rate of doing work’ means ‘work done divided by time’ (which is ‘power’)
5 Average acceleration = change in velocity/time taken
a = (30 m s–1 × 0 m s–1)/(8 s) = 4 m s–2
Chapter 71 The gradient of a displacement-time graph is the instantaneous velocity
The gradient of a velocity-time graph is the instantaneous acceleration
The area of a velocity-time graph is the change in displacement
The area of an acceleration-time graph is the change in velocity
2 Since body moves 20 m in 15 s and graph is a straight line
(a) (10 s/15 s) × 20 m = 13.3 m
(b) (8 m/20 m) × 15 s = 6.0 s
(c) Average speed = total distance/total time = 20 m/(15 s) = 1.3 m s–1
3 (a) Object is first accelerating, then constant velocity and then decelerating
(b) Stage 1
Acceleration = change in velocity/time = 12 m s–1/(5 s) = 2.4 m s–2
Distance = area under graph up to 5 s = 12
× 12 m s–1 × 5 s = 30 m
Stage 2
Acceleration = 0 m s–2 (since constant velocity)
Distance = area under graph from 5 s to 10 s = 12 m s–1 × 5 s = 60 m
Stage 3
Acceleration = –12 m s–1/(12 s) = –1 m s–2
Distance = area under graph from 10 s to 22 s = 12
× 12 m s–1 × 12 s = 72 m
(c) Total distance = 30 m + 60 m + 72 m = 162 m
Average speed = total distance/total time = 162 m/(22 s) = 7.4 m s–1
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions4
Acc
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–1.50 5 10 15 20 25
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0 1 2 3Time/s
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NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
Chapter 81 Record motion of ball in front of a vertical metre rule using a video camera
Replay the video a frame at a time and record displacement from scale at 0.04 s intervals
2
TimeVelo
city
Velo
city
/m s
–1
Time/s
Height of second bounce = either of the shaded areas
Acceleration of gravity = gradient of negative sloping lines
3
The two graphs are the same for the times for which the two balls are in the air
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
Time
Dis
plac
emen
t
Time
Velo
city
Time
Acc
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atio
n
4 Centre of the track (since both positive and negative displacements)
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Time
Dis
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t
Time
Velo
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Time
Acc
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Chapter 91 Using v = u + at
t = (v – u)/a = (18 m s–1 – 0 m s–1)/(4.5 m s–2) = 4.0 s
2 Using v = u + at
a = (v – u)/t = (0 m s–1 – 18 m s–1)/(4.5 s) = – 4.0 m s–2
Using x = 12
(u + v)t
x = 12
(18 m s–1 + 0 m s–1) × 4.5 s = 41 m
3 Using x = ut + 12
at2
x = (3.6 m s–1 × 4.5 s) + [12
× 1.4 m s–2 × (4.5 s)2] = 16.2 m + 14.2 m = 30.4 m
4 Using x = ut + 1–2 at2
u = (x – 12
at2)/t = 60 m – [12
× 35 m s–2 × (1.6 s)2]/(1.6 s) = (60 m – 44.8 m)/(1.6 s) = 15.2 m/(1.6 s) = 9.5 m s–1
Using v = u + at
v = 9.5 m s–1 + (35 m s–2 × 1.6 s) = 9.5 m s–1 + 56.0 m s–1 = 65.5 m s–1 = 66 m s–1
5
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5 (a) Using v2 = u2 + 2ax
a = [v2 – u2]/2x = [(9.0 × 105 m s–1)2 – (1.0 × 105 m s–1)2]/(2 × 0.20 m) = 2.0 × 1012 m s–2
(b) Using x = 12
(u + v)t
t = 2x/(u + v) = 2 × 0.20 m/(10.0 × 105 m s–1) = 4.0 × 10–7 s
Chapter 101 See pages 22 and 23
2 Using x = ut + 1–2 at2
from rest, x = 1–2 at2 = 12
× 9.81 m s–2 × (1.9 s)2 = 17.7 m
3 Using x = 12
at2 (from rest)
t = √(2x/a) = √[2 × 30 m/(9.81 m s–2)] = √(6.12 s2) = 2.5 s
Using v2 = 2ax (from rest)
v2 = 2 × 9.81 m s–2 × 30 m = 588.6 m2 s–2
v = √(588.6 m2 s–2) = 24.3 m s–1
4 Using v2 = u2 + 2ax and taking upwards as positive
u2 = v2 – 2ax = 02 – (2 × –9.81 m s–2 × 200 m) = 3924 m2 s–2
u = √(3924 m2 s–2) = 62.6 m s–1
Using x = 12
at2 (from rest)
Time to rise = time to fall = t = √(2x/a) = √[2 × 200 m/(9.81 m s–2)] = √(40.8 s2) = 6.4 s
Total distance travelled = 200 m + 200 m = 400 m
Final displacement = 0 m
5 (a) Using v = u + at
Speed = at = 150 m s–2 × 6 s = 900 m s–1
Distance = 12
at2 = 12
× 150 m s–2 × (6 s)2 = 2700 m
(b) Rocket then decelerates at 9.81 m s–2
Time to slow down = 900 m s–1/(9.81 m s–2) = 91.7 s
Total time to reach top = 6 s + 91.7 s = 97.7 s
Further distance covered = 450 m s–1 × 91.7 s = 41 284 m
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions(c)
Chapter 111 A body thrown horizontally from a cliff top takes the same time to reach the bottom as a body
dropped vertically. Provided air resistance is small, the horizontal velocity of a projectile is constantwhile its vertical velocity increases at 9.8 m s–2.
2 Using x = 12
at2 (from rest)
Time to fall t = √(2x/a) = √[2 × 0.85 m/(9.81 m s–2)] = √(0.173 s2) = 0.42 s
Time to fall t = √(2x/a) = √[2 × 2 m/(9.81 m s–2)] = √(0.408 s2) = 0.64 s
3 as Figure 11.3 on page 25 with h = 0.85 m and x = 6.4 m
Using x = 12
at2 (from rest) for the vertical motion
Time to fall t = √(2x/a) = √[2 × 0.85 m/(9.81 m s–2)] = √(0.173 s2) = 0.42 s
Since horizontal speed is constant
Speed = x/t = 6.4 m/(0.42 s) = 15.4 m s–1 = 15 m s–1
4 Using x = 12
at2 (from rest) for the vertical motion
Time to fall t = √(2x/a) = √[2 × 2 m/(9.81 m s–2)] = √(0.408 s2) = 0.64 s
Since horizontal speed is constant
x = speed × t = 400 m s–1 × 0.64 s = 255 m
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NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5 Using x =
12
at2 (from rest) for vertical motion of dart (falls 0.4 m vertically from rest)
t = √(2x/a) = √[2 × 0.4 m/(9.81 m s–2)] = 0.29 s
Since horizontal velocity is constant
Velocity = x/t = 3 m/(0.29 s) = 10.5 m s–1
Chapter 121 A force can cause a body to accelerate; either to speed up, to slow down or to change direction
2 The single force that could replace all other forces acting on a body and have the same effect
Maximum resultant force when forces act in same direction = 8 N + 12 N = 20 N
Minimum resultant force when forces act in opposite directions = 12 N – 8 N = 4 N
3 Both bodies have zero acceleration
So resultant force on each body must be zero
4 A body will remain at rest or continue to move with a constant velocity as long as the forces on itare balanced, i.e. the resultant force is zero
5 The inertia of a body is its reluctance to change velocity
Apply the same force to both stationary cans
The empty can will move the most as it has least inertia
Chapter 131 See page 28
2 Set up apparatus as described on page 28
Measure the mass of the trolley
Use a forcemeter to apply a constant force to the trolley and measure the resulting acceleration
Repeat for a range of known masses added to the trolley
Plot a graph of acceleration against 1/mass
A straight line through the origin shows that acceleration is directly proportional to 1/mass, soacceleration is inversely proportional to mass
3 Using F = ma
a = F/m = 24 000 000 N/(2 000 000 kg) = 12 m s–2
4 Using v = u + at
a = (v – u)/t = (40 m s–1 – 0 m s–1)/(10 s) = 4 m s–2
Using F = ma
F = 1200 kg × 4 m s–2 = 4800 N
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5 (a) Using F = ma
a = F/m = 150 N/(30 kg) = 5 m s–2
(b) Resultant force F = 150 N – 30 N = 120 N
a = 120 N/(30 kg) = 4 m s–2
Chapter 141 None
2 Both skaters have equal and opposite forces acting on them so move away from each other withaccelerations that depend on their masses; the heavier skater having the smaller acceleration
3 Whenever one body exerts a force on a second body, the second body always exerts a force on thefirst body; hence forces occur only in pairs
4 While body A exerts a force on body B, body B exerts an equal and opposite force on body A
5 A Newton III pair of forces cannot cancel each other as they act on different bodies
Chapter 151 Your weight arises from the gravitational attraction of the Earth pulling on you
The Newton III force that pairs with your weight is the gravitational attraction of you pulling on the Earth
2 Gravitational forces are always attractive while electromagnetic forces can be either attractive orrepulsive
3 Gravitational force of attraction between two masses
Electrostatic force of repulsion between two electrons
Magnetic force of attraction between two opposite poles
4 Gravitational, electromagnetic, strong nuclear and weak nuclear
5 Contact forces arise from electrostatic forces acting over very short distances
Chapter 161 Diagram showing a body with no forces acting on it
2 Similar to Figures 16.2 and 16.3 on page 34
Planet pulls the body down with a gravitational force
Body pulls the planet up with an equal gravitational force
3 While a body A exerts a force on a body B, body B exerts a force on body A. The forces are equal,opposite and of the same type; they have the same line of action and act for the same time
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
•••• Earth pushes chair up
•• I push chair down
• Earth pulls me down
•• Chair pushes me up
••• Chair pullsEarth up
•••• Chair pushes Earth down
• I pull Earth up
••• Earth pulls chair down
4 Joe pushes Fred right with a contact force of 40 N
5 See Figures 16.4, 16.5 and 16.6 on page 35
Chapter 171
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions2 Tension in cables
pulls crane down ••
Tension in cablespulls container up ••
Crane pushes Earth down •••
Container pullsEarth up
Crane pullsEarth up
• ••••
Earth pullscontainer ••••down
Earth pushescrane up •••
Earth pullscrane down •
3 Similarities: equal magnitude, same type, same line of action, act for the same time (any 2)
differences: opposite directions, act on different bodies
4 (a) Acting on same body
(b) Acting in same direction
(c) Different lines of action
(d) Different types of force
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5
Both forces act on the same body rather than on different bodies
Forces are of different types (gravitational down and contact up) rather than the same type
Forces produce equilibrium of book, a Newton III pair cannot oppose each other
Chapter 181 Total distance = 800 m + 1200 m + 300 m = 2300 m
As you end up being 500 m north and 1200 m east of your starting point:
Distance = √[(500 m)2 + (1200 m)2] = √(1 690 000 m2) = 1300 m
Angle east of north = tan–1 [1200 m/(500 m)] = tan–1 2.4 = 67°
2 8 m s–1 and 2 m s–1 are two perpendicular velocities
Resultant velocity = √[(8 m s–1)2 + (2 m s–1)2] = √(68 m2 s–2) = 8.2 m s–1
Angle to bank = tan–1 [8 m s–1/(2 m s–1)] = tan–1 4.0 = 76°
3 Resultant force = √[(14 N)2 + (9 N)2] = √(277 N2) = 17 N
Angle to 14 N force = tan–1 [9 N/(14 N)] = tan–1 0.64 = 33°This object is not in equilibrium as it has a resultant force of 17 N acting on it
800 m
1200 m
300 m
finaldisplacement
Book
Table pushes book upwith a contact force
Earth (and table) pullsbook down with
gravitational force
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions4 Split the SW force of 86 N into two components directed towards the South and the West:
86 N × cos 45° = 60.81 N towards the South
86 N × sin 45° = 60.81 N towards the West
Unbalanced force towards South = 60.81 N – 35 N = 25.81 N
Resultant force = √[(25.81 N)2 + (60.8 N)2] = √(4 363 N2) = 66 N
Angle below East = tan–1 [25.81 N/(60.8 N)] = tan–1 0.42 = 23°
5 When acting in same direction, resultant force = 25 N +14 N = 39 N
When acting in opposite directions, resultant force = 25 N – 14 N = 11 N
When these forces are perpendicular
Resultant force = √[(25 N)2 + (14 N)2] = √(821 N2) = 29 N
Angle to 25 N force = tan–1 [14 N/(25 N)] = tan–1 0.56 = 29°
Chapter 191
2 Vertical component = 220 N × cos 40° = 170 N
Horizontal component = 220 N × cos 50° = 140 N
3 (a) Force component = 85 N × cos 30° = 74 N
(b) Force component = 85 N × cos 55° = 49 N
(c) Force component = 85 N × cos 90° = 0 N
Vertical component
Horizontal component
4 Since pendulum is in equilibrium
Weight W = vertical component of tension = 35 N × cos 20° = 33 N
Force F = horizontal component of tension = 35 N × cos 70° = 12 N
5 Parallel component of tension = 600 N × cos 25° = 544 N
Perpendicular component of tension = 600 N × cos 65° = 254 N
Since moving with a constant velocity parallel to the tow path, resultant force is zero, so:
a force of 544 N must act backwards – produced by the water as the barge pushes it out of its path
a force of 254 N must act away from the bank – produced by an angled rudder
6 Vertical component of 60 N force = 60 N cos 30° = 52.0 N
Vertical component of 100 N force = 100 N cos 45° = 70.7 N
Horizontal component of 60 N force = 60 N cos 60° = 30.0 N
Horizontal component of 100 N force = 100 N cos 45° = 70.7 N
Total vertical force = 70.7 N – 52.0 N = 18.7 N down
Total horizontal force = 30 N + 70.7 N – 50 N = 50.7 N to the right
Resultant force = √[(50.7 N)2 + (18.7 N)2] = √(2920 N2) = 54 N
Angle = tan–1 [18.7 N/(50.7 N)] = tan–1 0.37 = 20° below the right-hand horizontal
For equilibrium, a fourth force of 54 N must act at 20° above the left-hand horizontal
Chapter 201 Upthrust is an upward force that acts on all immersed objects
Upthrust arises from the greater pressure acting on the bottom than on the top of an immersedobject
When in a river, part of the boulder’s weight is already opposed by the upthrust
Force required = weight – upthrust
2 Use apparatus as in Figure 20.2 on page 42
Time how long it takes for ball bearing to pass through each equal length section
Times will decrease but then become constant
Constant times show that the ball bearing has reached its terminal speed
3 Using v2 = u2 + 2ax
From rest v2 = 2ax = 2 × 9.81 m s–2 × 1000 m = 19 620 m2 s–2
v = √(19 620 m2 s–2) = 140 m s–1
Other forces acting are upthrust and drag
As the speed of a raindrop increases so do the drag forces acting on it
Resultant force on the raindrop = weight – (upthrust + drag)
Resultant force on the raindrop decreases as its speed increases, becoming zero before drop’s speedreaches anywhere near 10 m s–1
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
4 Air has to travel faster over the curved upper wing surface than the flat lower surface
Air pressure is least where the air travels fastest
The pressure difference produces the upward force known as aerodynamic lift
The upside-down wing on a racing car produces a downward force that improves the grip betweenthe tyres and the track
5 See Figure 20.7 on page 43
Drag = thrust
Lift = weight
Horizontally:
forward components of thrust and lift = backward component of drag
Vertically:
upwards components of lift and drag = weight + downward component of thrust
air pushesaircraft (lift)
Earth pulls aircraft(weight)
air pushes aircraft(thrust)
air pushesaircraft (drag)
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 211
2 (a) The ground/starting blocks push the athlete forwards
The force arises as the athlete pushes backwards on the ground/starting blocks
(b) Constant velocity so no acceleration and horizontal forces must balance
Ground pushes athlete
Earth pulls athlete
Air pushes athlete (drag) Ground pushes athlete
Earth pulls book down
Table pushes book up
Book pushes table down
Earth pullstable down
Earth pushes table up
man pushesbox to right
friction with Earth’ssurface pushes boxto left
Earth pulls boxdown (gravitational)
Earth pushes box up(contact)
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsEarth
pulls carAir
pulls car
Groundpushes car
Groundpushes car
Groundpushes car
Trailerpulls car
Car pulls trailer Earth pulls trailer
Friction fromEarth’s surfacepushes trailer
Normal forcesfrom Earth’s surface
pushes trailer
3
4
(a) Forces on box must balance in both horizontal and vertical directions
(b) Force from man pushing box is greater than frictional force from floor on box
5
Lamp is stationary so resultant force on it must be zero
Chapter 221
Moment about centre of wheel = (18 N × 0.18 m) + (18 N × 0.18 m) = 6.5 N m
2 The moment of a force is the product of force and its perpendicular distance from the point aboutwhich the force is acting
A torque is the resultant moment of two or more turning forces
3 (a) Moment = F × perpendicular distance = 20 N × 0.40 m = 8.0 N m
(b) Perpendicular distance from P = 0.60 m × sin 65° = 0.54 m
Moment = F × perpendicular distance = 35 N × 0.54 m = 19 N m
18 N
18 N
Earth pulls lamp
Tension pulls lamp Tension pulls lamp
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
4 If a body is in equilibrium, the sum of the moments about any point must be zero
Sum of the moments about:
left-hand support = (35 kN × 24 m) – (10.5 kN × 80 m) = 840 kN m – 840 kN m = 0
right-hand support = (35 kN × 56 m) – (24.5 kN × 80 m) = 1960 kN m – 1960 kN m = 0
centre = (35 kN × 16 m) + (10.5 kN × 40 m) – (24.5 kN × 40 m) = 560 kN m + 420 kN m – 980 kN m = 0
5 For beam to balance, sum of moments about its pivot is zero:
16 N × 25 cm = (a) × 10 cm
(a) = 400 N cm/(10 cm) = 40 N
3 N × (b) = 5 N × 18 cm
(b) = 90 N cm/(3 N) = 30 cm
35 N × 8 cm = 14 N × (c)
(c) = 280 N cm/(14 N) = 20 cm
(d) × 18 cm = 45 N × 16 cm
(d) = 720 N cm/(18 cm) = 40 N
Chapter 231 The point at which all the weight of the body appears to act
See experiment at top of page 48
2 Condition 1: the sum of the forces in any direction is zero
Condition 2: the sum of the moments about any point is zero
Usually condition 1 is applied to two perpendicular directions to produce two equations andcondition 2 used to produce the third equation
3 Foot of ladder is 3 m from base of wall √[(5 m)2 – (4 m)2]
Sum of vertical forces is zero:
R2 – 150 N = 0 … equation (1)
Sum of horizontal forces is zero:
R1 – F = 0 … equation (2)
Sum of moments about point of contact of ladder with floor is zero:
R1 × 4 m = 150 N × 1.5 m
R1 × 4 m = 225 N m … equation (3)
From equation (1), R2 = 150 N
From equation (3), R1 = 225 N m/(4 m) = 56 N
From equation (2), F = R1 = 56 N
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
4m
R1
1.5m
150N
F
R2
4 Rule 1: when the three forces are drawn as head-to-tail vectors, they form a closed triangle
Rule 2: all three forces must pass through the same point
Note that the intersection of lines of action of F and W determine the common point through whichthe third force must act
5 W (N) 2.0 3.0 4.0 5.0 6.0 7.0 8.0
x (cm) 52 35 26 21 17 15 13
1/x (m–1) 1.92 2.86 3.85 4.76 5.88 6.67 7.69
Weight of stand = gradient of graph/(0.08 m) = 1.04 N m/(0.08 m) = 13 N
Chapter 241 See second experiment on page 50
Precautions:
balance rule accurately before adding masses
balance screw on its head, using the slot in its head to position it accurately on the rule’s scale
similarly use any slot in 10 g mass to assist in its accurate positioning
use a range of large distances from the pivot
0 1 6(1/x)/m–1
W/N
2 3 4 5 7 8
8
7
6
5
4
3
2
1
0
gradient=Wx=1.04N m
force fromtop hinge
W
F
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions2
For vertical equilibrium, vertical component of tension = weight of sphere = 25 N
Vertical component of tension = T × cos 30°T = 25 N/(cos 30°) = 29 N
For horizontal equilibrium, horizontal component of tension = horizontal force F
Horizontal component of tension = T × cos 60°F = 29 N × cos 60° = 14 N
3 Line of action of painter’s weight is 2.4 m from foot of ladder 3 m × 4 m/(5 m)
Sum of vertical forces is zero:
R2 – 150 N – 750 N = 0
R2 – 900 N = 0 … equation (1)
Sum of horizontal forces is zero:
R1 – F = 0 … equation (2)
Sum of moments about point of contact of ladder with floor is zero:
R1 × 4 m = (150 N × 1.5 m) + (750 N × 2.4 m)
R1 × 4 m = 225 N m + 1800 N m
R1 × 4 m = 2025 N m … equation (3)
From equation (1), R2 = 900 N
From equation (3), R1 = 2025 N m/(4 m) = 510 N
From equation (2), F = R1 = 510 N
30˚
tensionin string (T)
weight(25N)
horizontalforce (F)
4m
R1
1.5m
150N
F
R2
2.4m750N
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions4 Taking moments about P
T2 × 2.2 m = 150 N × 1.2 m = 180 N m
T2 = 180 N m/(2.2 m) = 82 N
For vertical equilibrium
T1 + T2 = 150 N
T1 = 150 N – 82 N = 68 N
5 The figure shows the forces acting on the rod
Clockwise moment about hinge = 90 N × 1.5 m = 135 N m
For equal anticlockwise moment, Tvertical = 135 N m/(1.5 m) = 90 N
Tvertical × 1.5 m = 135 N m
Tvertical = 135 N m/(1.5 m) = 90 N
Angle wire makes with vertical = tan–1 1.5 m/(0.9 m) = tan–1 1.67 = 59°
T × cos 59° = 90 N
T = 90 N/(cos 59°) = 175 N
Horizontal component of tension = T × cos 31° = 175 N × cos 31° = 150 N
For horizontal equilibrium (only two forces have horizontal components):
Horizontal force of hinge = horizontal component of tension = 150 N
For vertical equilibrium:
weight acting down = 90 N
vertical component of tension acting up = 90 N
So vertical force of hinge = 90 N – 90 N = 0 N
0.9 m
90 N
hinge
Fv
Fh
T
1.5 m
P
0.3 mT1
2.2 m 0.5 m
1.2 m 1.0 m
150 N
T2
6 Taking moments about A
T2 × 1.2 m = (100 N × 0.5 m) + (250 N × 0.6 m) + (350 N × 1.0 m)
T2 × 1.2 m = 50 N m + 150 N m + 350 N m = 550 N m
T2 = 550 N m/(1.2 m) = 460 N
For vertical equilibrium
T1 + T2 = 100 N + 250 N + 350 N = 700 N
T1 = 700 N – 460 N = 240 N
Chapter 251 Momentum = mass × velocity
Momentum is a vector quantity
2 Momentum = mass × velocity
(a) Momentum of rugby player = 120 kg × 10 m s–1 = 1200 kg m s–1
(b) Momentum of electron = 9 × 10–31 kg × 2 × 107 m s–1 = 1.8 × 10–23 kg m s–1
(c) Momentum of toy train = 1.6 kg × 0.25 m s–1 = 0.4 kg m s–1
3 Change in momentum = final momentum – initial momentum = mv – mu
(a) Change in momentum of car = (800 kg × 30 m s–1) – (800 kg × 5 m s–1) = 24 000 kg m s–1 – 4000 kg m s–1 = 20 000 kg m s–1
(b) Change in momentum of trolley = (0.8 kg × 0.2 m s–1) – (0.8 kg × 0.8 m s–1) = 0.16 kg m s–1 – 0.64 kg m s–1 = – 0.48 kg m s–1
(c) Change in momentum of ball = (0.05 kg × –5 m s–1) – (0.05 kg × 7 m s–1) = – 0.25 kg m s–1 – 0.35 kg m s–1 = – 0.6 kg m s–1
4 The rate of change in momentum of a body is directly proportional to the resultant force acting onit and takes place in the same direction as the resultant force
Force ∝ rate of change in momentum
F ∝ (mv – mu)/t ∝ m(v – u)/t ∝ ma
F = kma where k is the constant of proportionality
In SI units, the newton is defined so that k = 1, so F = ma
0.5 m
T1
A
100 N
250 N
0.4 m0.1 m
B
350 N
T2
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5 Force = change in momentum/time
(a) Force acting on car = 20 000 kg m s–1/(8 s) = 2500 N
(b) Force acting on trolley = – 0.48 kg m s–1/(3 s) = – 0.16 N
(c) Force acting on ball = – 0.6 kg m s–1/(0.6 s) = –1 N
Chapter 261 Provided no external forces act, the total momentum in any direction remains constant so that the
total momentum after the collision equals the total momentum before the collision
See experiment on page 54
2 Momentum of skateboard = mu = 4 kg × 2 m s–1 = 8 kg m s–1
Combined mass after bag lands on it = 4 kg + 1 kg = 5 kg
Assuming momentum is unchanged
5 kg × v = 8 kg m s–1
v = 8 kg m s–1/(5 kg) = 1.6 m s–1
3 Momentum of bullet = mu = 0.02 kg × 300 m s–1 = 6 kg m s–1
Since block is stationary, total initial momentum (TIM) = 6 kg m s–1
Total final momentum (TFM) = TIM = 6 kg m s–1 (since momentum conserved)
Final speed = TFM/(total mass) = 6 kg m s–1/(4 kg) = 1.5 m s–1
4 TIM = (65 kg × 7 m s–1) + (45 kg × – 6 m s–1)
TIM = 455 kg m s–1 – 270 kg m s–1 = 185 kg m s–1
TFM = TIM = 185 kg m s–1
Combined speed = TFM/(total mass) = 185 kg m s–1/(110 kg) = 1.7 m s–1
In the original direction of the 65 kg skater
5 Prior to a gun being fired, its total momentum is zero (TIM = 0)
As momentum is conserved, total momentum after firing must also be zero (TFM = 0)
Pellet has momentum in the forward (positive) direction
so gun must have momentum in the backward (negative) direction, and so recoils
6 (a) Momentum of stone = mu = 0.1 kg × 6 m s–1 = 0.6 kg m s–1
(b) TFM = TIM = 0.6 kg m s–1
Speed of squirrel = TFM/(total mass) = 0.6 kg m s–1/(0.6 kg) = 1 m s–1
(c) Total momentum must remain at 0.6 kg m s–1
Stone’s new momentum = 0.1 kg × –2 m s–1 = – 0.2 kg m s–1 (as backwards)
Squirrel’s momentum = (0.6 + 0.2) kg m s–1 = 0.8 kg m s–1 (to keep TFM = 0.6 kg m s–1)
Squirrel’s final speed = 0.8 kg m s–1/(0.5 kg) = 1.6 m s–1
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 271 Impulse = force × time
Unit of impulse from this equation is N s
In base units:
N s = kg m s–2 × s = kg m s–1
The same unit as momentum
2 (a) Impulse = Ft = 60 N × 0.008 s = 0.48 N s
(b) Ft = mv – mu but since u = 0, Ft = mv
v = Ft/m = 0.48 N s/(0.15 kg) = 3.2 m s–1
3 Impulse = area under force-time graph
Impulse = 12
× 6 N × (0.3 s + 0.9 s) = 3.6 N s
Impulse = Ft = mv – mu but since u = 0, Ft = mv
v = Ft/m = 3.6 N s/(0.8 kg) = 4.5 m s–1
4 (a) Change in momentum = mv – mu = m(v – u) = 900 kg (0 m s–1 – 30 m s–1) = –27 000 kg m s–1
(b) Impulse of wall on car = mv – mu = –27 000 N s
(c) Force of wall on car F = impulse/t = –27 000 N s/(0.5 s) = –54 000 N
5 (a) Change in momentum = m(v – u) = 0.3 kg (–2 m s–1 – 8 m s–1) = 0.3 kg × –10 m s–1
= –3 kg m s–1
(b) Impulse of hammer on nail = mv – mu = –3 N s
(c) Force of hammer on nail F = impulse/t = –3 N s/(0.012 s) = –250 N
(d) Connect one of the ‘start’ leads of a digital timer to the nail and the other to the metal hammer head
6 When two bodies collide, they exert equal and opposite forces on each other, F and –F
These forces act for the same length of time t
Therefore the impulses are also equal and opposite, Ft and –Ft
and the change in momentum of one body is equal and opposite to the change in momentum ofthe other
So the overall change in momentum is zero and total momentum is conserved
7 TIM = 3 kg × 4 m s–1 = 12 kg m s–1
TFM = TIM = 12 kg m s–1
Momentum of 2 kg sphere after collision = 2 kg × 4.5 m s–1 = 9 kg m s–1
Momentum of 3 kg sphere = 12 kg m s–1 – 9 kg m s–1 = 3 kg m s–1
Speed of 3 kg sphere = momentum/mass = 3 kg m s–1/(3 kg) = 1 m s–1
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 281 Work = force × distance moved in the direction of the force
(a) Work = 60 N × 3 m = 180 J
(b) Work = 4000 N × 0.25 m = 1000 J
2 (a)Work done = area under graph up to 60 mm = 12
× 1.5 N × 0.06 m = 0.045 J
(b) Work done = area under graph between 40 mm and 140 mm=
12
× (1.0 N + 3.5 N) × (0.14 m – 0.04 m) = 0.225 J
3 Work done = area under graph
Area up to 3 cm ≈ 12
× 0.03 m × 13.6 N ≈ 0.20 J
Area between 3 cm and 9.5 cm ≈ 0.065 m × 14.2 N ≈ 0.90 J
Total work done ≈ 1.1 J
4 Power is the rate of doing work
(a) Average speed = distance/time = 36 m/(60 s) = 0.60 m s–1
(b) Average upward velocity = upward displacement/time = 21 m/(60 s) = 0.35 m s–1
(c) Total work done against his weight = weight × height = 800 N × 21 m = 16 800 J
(d) Average power = work/time = 16 800 J/(60 s) = 280 W
5 144 km h–1 = 144 000 m h–1/(60 × 60 s h–1) = 40 m s–1
Power = force × velocity
Resistive force = power/velocity = 35 000 W/(40 m s–1) = 875 N
Chapter 291 Energy is a scalar quantity
Base units: J = N m = kg m s–2 m = kg m2 s–2
2 Energy can be stored as either potential energy or kinetic energy
3 types of potential energy: gravitational, electromagnetic and nuclear
elastic potential energy
3 Increase in gravitational potential energy ∆W = mg∆h
(a) ∆W = 0.5 kg × 9.81 N kg–1 × 25 m = 123 J
(b) ∆W = 60 kg × 9.81 N kg–1 × 0.30 m = 177 J
(c) ∆W = 1.2 × 10–6 kg × 9.81 N kg–1 × 0.15 m = 1.8 × 10–6 J
4 Kinetic energy = 12
mv2
Kinetic energy of car = 12
× 900 kg × (20 m s–1)2 = 180 000 J
If all kinetic energy is converted into gravitational potential energy, mgh
Height risen h = kinetic energy/(mg)
h = 180 000 J/(900 kg × 9.81 N kg–1) = 20.4 m
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions5 (a) Kinetic energy of trolley =
12
× 0.60 kg × (0.85 m s–1)2 = 0.22 J
h = 0.22 J/(0.60 kg × 9.81 N kg–1) = 0.037 m
(b) Kinetic energy of ball = 12
× 0.11 kg × (40 m s–1)2 = 88 J
h = 88 J/(0.11 kg × 9.81 N kg–1) = 82 m
not surprisingly, the worked example gives the same height!
Chapter 301 In this situation, the decrease in the gravitational potential energy corresponds to an increase in the
internal energy of the object and its surroundings due to the frictional forces acting on it
2 The internal energy of a body is the total of the random kinetic and potential energies of all themolecules of that body
Internal energy may be increased by:
mechanical working by hammering
electrical working by the passing of an electric current
heating in a hot fire
3 The energy content of a closed or isolated system remains constant
4 (a) Potential energy lost by falling mass = mg∆h = 1 kg × 9.81 N kg–1 × 0.25 m = 2.45 J
(b) Total kinetic energy just before hitting ground = potential energy lost by falling mass
12
(m1 + m2)v2 = 2.45 J
v2 = 2 × 2.45 J/(1 kg + 4 kg) = 0.98 m2 s–2
v = √(0.98 m2 s–2) = 0.99 m s–1
5 Efficiency = useful output/input
Power of light emitted = (2/100) × 60 W = 1.2 W
The other 58.8 W increases the internal energy of the surroundings
Chapter 311 See experiment on page 54
2 Momentum and energy are conserved in both elastic and inelastic collisions
Elastic collisions also conserve kinetic energy; inelastic collisions do not
The collisions between the molecules of a gas are, on average, elastic
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions3 TIM = mu = 4 × 104 kg × 3 m s–1 = 1.2 × 105 kg m s–1
TFM = TIM = 1.2 × 105 kg m s–1
Speed after collision = TFM/(total mass) = 1.2 × 105 kg m s–1/(6 × 104 kg) = 2 m s–1
Kinetic energy after collision = 12
× 6 × 104 kg × (2 m s–1)2 = 1.2 × 105 J
Kinetic energy before collision = 12
× 4 × 104 kg × (3 m s–1)2 = 1.8 × 105 J
This shows that the collision was inelastic, 6 × 104 J is spread around, mainly raising the internalenergy of the buffers and surroundings so that energy is still conserved
4 Gravitational potential energy → kinetic energy → gravitational potential energy → kinetic energy→ gravitational potential energy
5 (a) Momentum of bullet = mu = 0.02 kg × 300 m s–1 = 6 kg m s–1
Since block is stationary before collision, TIM = 6 kg m s–1
Since momentum is conserved, TFM = TIM = 6 kg m s–1
Combined speed = TFM/(total mass) = 6 kg m s–1/(4 kg) = 1.5 m s–1
(b) Kinetic energy of bullet = 12
mu2 = 12
× 0.02 kg × (300 m s–1)2 = 900 J
Kinetic energy of block and bullet = 12
Mv2 = 12
× 4 kg × (1.5 m s–1)2 = 4.5 J
Collision is inelastic as kinetic energy is not conserved
99.5% of bullet’s kinetic energy is converted to other forms
6 Motorway crash barriers are designed to absorb the kinetic energy of any vehicle that hits them toprevent the vehicle from bouncing back into the carriageway
Chapter 321 neutron neutral
proton positive
electron negative
2 An atom consists of a very small central nucleus where most of its mass is concentrated and aroundwhich low-mass electrons orbit
Beryllium-8 has 4 protons and 4 neutrons in its nucleus with 4 orbiting electrons
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions3 Density = mass/volume
An atom is mostly empty space with no mass
Nearly all the mass is concentrated into a very small central volume (very large nuclear density)
The overall density is an average for the whole material, taking into account the empty space
4 (a) number of protons = 82
(b) number of nucleons = 207
(c)number of neutrons = 207 – 82 = 125
5 Isotopes are nuclides with the same number of protons but a different number of neutrons
Lightest (1st) isotope of tin is Sn-108 i.e. (107 + 1)
2nd isotope of tin is Sn-109 i.e. (107 + 2)
3rd isotope of tin is Sn-110 i.e. (107 + 3)
So 25th isotope of tin is Sn-132 i.e. (107 + 25)
Possible symbols: 10950Sn, 110
50Sn ...... 13150Sn, 132
50Sn
Chapter 331 See Figure 33.2 on page 70
The vast majority of alpha particles are deflected very little as they travel through the gold foil
while a tiny minority (about 1 in 8000) are deflected through angles greater than 90°
2 See Figure 33.3 on page 70
The positive nuclei have comparatively large distances between them so most alpha particles aredeflected very little
The closer the path of an alpha particle comes to a nucleus, the more the alpha particle is deflected
Deflections through angles greater than 90° result from almost head-on collisions
3 Diameter of an atom ≈ 3 × 10–10 m
Diameter of a nucleus ≈ 1 × 10–14 m
∴ The diameter of this atom is about 30 000 times greater than the diameter of this nucleus
Area of circle ∝ diameter2
∴ The head-on area of this atom is about 30 0002 times greater than the head-on area of this nucleus
Percentage taken up by nucleus = 100 × 1/(30 000)2 ≈ 0.000 000 1% (which is why so many alphaparticles miss!)
4 Quarks are the particles from which all sub-atomic particles are made
There are six types of quark called up, down, strange, charm, top, bottom
A proton consists of two up quarks and one down quark
A neutron consists of one up quark and two down quarks
A baryon is a particle made up of three quarks
A meson is a particle made up of a quark and an antiquark
5
Chapter 341 When ionised, an atom releases an electron and becomes a positively charged ion
Air can be ionised either by a flame or by the radiation from a radioactive source
2 See second experiment on page 72
3 21584Po → 211
82Pb + 42α22789Ac → 223
87Fr + 42α
4
Smoke particles in air reduce the number of alpha particles reaching ‘the detector’
fewer ionisations then occur within ‘the detector’
so a lower current flows when smoke is present
A reduction in the current is used to trigger the alarm
5 22890Th → 224
88Ra + 42αTo get to lead-212 from radium-224, 12 nucleons must be removed
as each alpha particle removes 4 nucleons (and beta removes none), 3 more alpha decays are required
the proton number of all isotopes of lead is 82
Chapter 351 A GM tube is more sensitive: it can detect any single ionising event that occurs inside the tube while
an ionisation chamber needs a large number of ionising events to produce a measurable current
A GM tube allows each ionising event to be directly registered on a counter
A GM tube detects radiation once it has entered the tube through its walls (it is poor at detectingalpha radiation that is mostly stopped by the walls) while the radioactive source can be placeddirectly inside an ionisation chamber
2 Place source close to GM tube window
Observe count rate as paper placed between source and GM tube – no change, no alpha
Repeat with aluminium instead of paper – reduction in count rate, beta being emitted
Repeat with lead instead of aluminium – no emissions from source detected, no gamma
Alphasource
Alpha particledetector
Air gap
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
deep inelastic scattering alpha particle scattering
Incident particles electrons alpha particles
Targets protons/neutrons atoms in foil
Process deflections off smaller parts within nucleons deflections off smaller parts within atoms
Results quarks discovered nucleus discovered
3 In beta-minus decay, a neutron in the nucleus splits into a proton and an electron10n → 1
1p + –10e
The proton stays in the nucleus but the electron is ejected at high speed as a beta-minus particle
4 21684Po → 212
82Pb + 42α212
82Pb → 21282Pb + γ
21282Pb → 212
83Bi + –10β
5
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice Questions
Pu24194
0
–1Am241
95
42
Np23793
42
Pa23391
0
–1U233
92
42
Th22990
42
Ra22588
0
–1Ac225
89
42
Fr22187
42
At21785
Bi21383
0
–1Po213
84
42
Pb20982
0
–1Bi209
83
42
NAS Physics Teachers’ Guide © 2005 Nelson Thornes Ltd.
Unit 1Mechanics and Radioactivity
Solutions to Practice QuestionsChapter 361 Background radiation is the radiation that is around us all the time
natural radioactivity is associated with isotopes that occur naturally
artificial radioactivity is associated with isotopes produced by man by neutron bombardment
cosmic rays are another important contributor to background radiation
2 Radioactive decay is a random process as it is impossible to predict when an individual atom will decay
A radioactive source contains an extremely large number of atoms
The unpredictable individual decays of such a large number together produce a statistical patternfrom which predictions can be made
3 Activity is the number of decays of a radioactive source per second
Decay constant is the probability of decay per nucleus per second
Activity = λN
Activity = 8.0 × 10–6 s–1 × 3.0 × 1011 = 2.4 × 106 s–1
As nuclei decay, there are fewer and fewer nuclei left to decay so the decay rate decreases
4 Half-life is the average time taken for half the nuclei of that isotope to decay
See experiment on page 78
5 t = ln 2/λt = ln 2/λ = 0.69/(7.84 × 10–10 s–1) = 8.80 × 108 s = 8.80 × 108 s/(60× 60 × 24 × 365.25 s y–1)
= 27.9 y
84 years = 3 × 28 years = 3t
Mass of strontium isotope will have fallen to (12
)3 = 1/8
Mass = 4.5 mg × 1/8 = 0.56 mg
12
12
12