Thames & Kosmos PHYSICS pro Experiment Manual

Page 1
EXPERIMENT MANUAL
Franckh-Kosmos Verlags-GmbH & Co. KG, Pfizerstr. 5-7, 70184 Stuttgart, Germany | +49 (0) 711 2191-0 | www.kosmos.de Thames & Kosmos, 301 Friendship St., Providence, RI, 02903, USA | 1-800-587-2872 | www.thamesandkosmos.com Thames & Kosmos UK Ltd, Goudhurst, Kent, TN17 2QZ , United Kingdom | 01580 212000 | www.thamesandkosmos.co.uk
Page 2
KIT CONTENTS
The parts in your kit:
GOOD TO KNOW !
parts, please contact Thames & Kosmos
customer service. Any materials not included in the kit are indicated in italic script under
the “You will need” heading.
If you are missing any
32 25
7
43
24
21
8
23
30
16
17
18
1
5 3 2
4
411211
13 31 22
9
10
26
42
20
36
35
6
29 37
33
14
15
28
19
39
38
No. Description Count Item No.
1 Anchor pin 40 702527 2 Joint pin 12 702524 3 Shaft plug 30 702525 4 Shaft pin 2 702526 5 Axle lock 12 702813 6 Washer 12 703242 7 Long frame 4 703239 8 Short frame 6 703232 9 Long rod 6 703235 10 Short rod 6 703233 11 Long axle 4 703234 12 Medium axle 5 703238 13 Short axle 1 703236 14 Medium pulley wheel 4 702518 15 Small pulley wheel 4 702519 16 Large gear wheel (60 teeth) 2 702506 17 Medium gear wheel (40 teeth) 4 702505 18 Small gear wheel (20 teeth) 7 702504 19 Baseplate 2 703237 20 Crankshaft 2 702599 21 XL (extra long) axle 1 703518 22 Connector bridge 2 703231 23 Turbine blade 16 702815
No. Description Count Item No.
24 Rubber band (long) 1 703241 25 Rubber band (medium) 1 703374 26 Cotton cord (white) 1 703244 28 Wheel 2 703230 29 Tire ring (medium pulley wheel) 2 703251 30 Anchor pin lever 1 702590
(Part separator tool)
31 Crank 2 703377 32 Straw (red) 2 703513 33 Digging shovel 1 703514 34 Experiment book (not shown) 1 703510 35 Measuring cup 1 703532 36 Plastic strip for spring motor 1 703240 37 Film for cutouts 1 703380 38 Boat hull 1 703519 39 Die-cut cardboard sheets 1 703522 40 Hydraulic pump 1 703515 41 Hydraulic switch 1 703516 42 Hydraulic cylinder 4 703378 43 Narrow tubing 1 703500 44 Thick tubing 1 703511
3
Page 3
Air and Water in the Flow
19
20
22
3
23
21
3
24
39
Page 4
GOOD TO KNOW
P (Pressure) =
F
1
: A
1
= F
2
: A
2
p
1
: p
2
= V
2
: V
1
p
1
: p
2
= T
1
: T
2
or: p · V = constant
(only valid when T = constant)
F
1
· L
1
= F
2
· L
2
p
1
· V
1
= p
2
· V
2
A
1
· v
1
= A
2
· v
2
Load · Load arm = Force · Force arm
F (Force)
A (Area)
F
d
=C
d
·
A · · v
2
2
P == 2= 2 Pa
10 N 5 m
2
N
m
2
P == 200,000 Pa
100 N
0.0005 m
2
P =
= 16,000 Pa or 16 hPa or 1.6 bar
4 N
0.00025 m
2
or = constant=
1
p · V
T
p
2
· V
2
T
2
F
d
= 0.4 ·
2 m
2
· 1.23 kg/m
3
· (40 m/s)
2
2
F
d
= 0.4 ·= 787.2 N
3936
2
kg · m
s
2
Total energy
Work yielded
Friction
Slip-
stream
Turbulence
Panel
Cylinder
Teardrop
Turbulence
Toggle switch center Stop in all directions
Supply
Toggle switch
left
Toggle switch
right
A1
V1
V2
Equal quantities of water
A2
Total Pressure
Dynamic Pressure
Static Pressure
Air and Water in the Flow
THE FLOW EQUATION
If you multiply the large cross­sectional area (A1) by the corresponding velocity (v1), the product is the same as when you multiply the small cross-sectional area (A2) by the velocity there (v2).
Pressure in currents
Because the speed of the water increases in the narrow part of a tube, the pressure also increases in the direction of flow. But an increase in pressure also means an increase in force per unit of area and, thus, an increase in the distance the narrower stream of water can shoot.
The pressure in the direction of flow is also called dynamic pressure, because it arises with dynamics, or the force of movement. In tubes, there is always also something called static (resting) pressure, which is a product of the difference in pressure between the entrance to and exit from the tube.
Dynamic pressure is measured against the stream, static
pressure in the stream. When the liquid is resting, there is only static pressure, and the dynamic pressure is equal to zero. When movement starts, dynamic pressure rises and static pressure simultaneously drops.
That also applies in reverse. In a uniform current, in any case, the sum of the two pressures is always the same.
This equation is called the flow rate equation or continuity equation:
45
Page 5
EXPERIMENT 18
Total energy
Work yielded
Friction
Toggle switch center Stop in all directions
Supply
Toggle switch
left
Toggle switch
right
= F
2
: A
2
p
1
: p
2
= V
2
: V
1
p
1
: p
2
= T
1
: T
2
or: p · V = constant
F
1
· L
1
= F
2
· L
2
p
1
· V
1
= p
2
· V
2
A
1
· v
1
= A
2
· v
2
F (Force)
A (Area)
P (power) =
W (work)
t (time)
F
d
=C
d
·
A · · v
2
2
P == 2= 2 Pa
10 N
5 m
2
N m
2
P == 200,000 Pa
100 N
0.0005 m
2
P =
= 16,000 Pa or 16 hPa or 1.6 bar
4 N
0.00025 m
2
or = constant=
p · V
T
p
2
· V
2
T
2
F
d
= 0.4 ·
2 m
2
· 1.23 kg/m
3
· (40 m/s)
2
2
F
d
= 0.4 ·= 787.2 N
3936
2
kg · m
s
2
1 N =
1 kg · m
s
2
1 Pa =
1 bar = 1,000 hPa
1 N
1 m
2
1 W =
1 J
1 s
P (Pressure) =
F
1
: A
1
= F
2
: A
2
F
1
· L
1
= F
2
· L
2
Load · Load arm = Force · Force arm
F (Force)
A (Area)
P == 2= 2 Pa
10 N 5 m
2
P == 200,000 Pa
100 N
0.0005 m
P =
= 16,000 Pa or 16 hPa or 1.6 bar
0.00025 m
Compressed air
The air-filled balloon has potential energy too. You can drive a paddle wheel turbine with it.
1
 x
23
17
YOU WILL NEED
 Axle lock
 Washer
 Short frames
 Long axle 
 Medium gear wheels 
 Baseplate 
 Turbine blades 
› 1 Balloon
2
Water, Air, and Energy
CONSERVATION OF ENERGY
Not all of the potential energy of the water is converted into hammer beats in our gravity hammer experiment. Part of it is used up by friction in the axle seats, the pulley wheels, and the hammer shaft. In this process, it is only lost as far as the hammering is concerned. If you add up the work from the friction and the hammering, it equals the energy you started with.
Power is work divided by time
Balloon
Work is measured independent of the time it takes to do the work. If
3
you do the same amount of work in less time, then you exert more power doing it — whether its raising your hand in school or biking.
When you calculate power, time becomes a factor. Power is the relationship of the work performed to the time needed to do it:
The unit of measure for power P is the watt (W):
8
19
17
11
6
5
In other words, the conservation of
energy law applies:
In addition to watts, kilowatts (1 kW = 1,000 W) and megawatts (1 mW = 1,000,000 W) are also used as units of power. The engine of a mid-sized car handles about 60 kW. A human can perform about 200 watts of physical work over a long period of time, while a cyclist with a bicycle can get to 1,500 watts fairly quickly.
In a closed mechanical
system, no energy is lost. Energy can be neither created nor destroyed. It can only be converted. The sum of the
mechanical energy remains the same (constant).

Page 6
CAR WITH HYDRAULIC BRAKES
Let‘s Build Models
Every vehicle should be able to brake. As their main braking device, passenger cars have a hydraulically activated foot brake. Its hydraulic mechanism consists of a cylinder that transfers force from the
brake pedal to the main cylinder. From there, the braking force is transferred equally by separate pathways to the braking cylinders on the wheels. Big and heavy vehicles, e.g. a tour bus or dredger, have so-called servo brakes, which amplify the braking force through a pump.
This model is like the racing car model (page 89) — but without the drive spring. Test the hydraulic brake by pushing against the car’s brake pedal (the front pair of rods). Push the pedal down to activate the brake. That pulls the rear pair of rods down onto the tires. Water will serve as the hydraulic fluid. You will see in Experiments 1 and 2 (on pages 10 and
11) how to fill it without air bubbles.
> See Pages 10-11 and 20-22
YOU WILL NEED
8 Anchor pins 14 Joint pins 2 2 Shaft plugs 310 Axle locks 5 8 Washers 61 Short frame 84 Long rods 96 Short rods 104 Long axles 113 Medium axles 122 Medium pulleys 142 Large gear wheels 162 Small gear wheels 181 XL (extra long) axle 211 Rubber band (medium) 252 Wheels 282 Tire rings for pulleys 29 2 Hydraulic cylinders 421 Piece of narrow tubing 43
1
2
3
10 11
42
4
1
1
9
2
12
42
12
5
43
5
6
5
10
1
65
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