Connected Particles

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Connected Particles

By a connection, we mean a system where multiple particles are linked by another force. For example, a car pulling a caravan is connected by the coupling, which provides tension on both objects.

Make sure you are happy with the following topics before continuing.

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Assumptions

First off, we have to assume that pulleys, pegs and other potential external factors are smooth, unless explicitly told otherwise.

We’ll also treat multiple connected particles as one mass, with the same velocity and acceleration. Without this, we could assume the connection has failed between the two particles, i.e. a linked piece of string has snapped, or slackened.

We’re also going to assume that Newton’s Laws hold, especially the Second Law, F=maF = ma. In fact, we’re going to use F=maF = ma in the direction that each particle moves individually.

Otherwise, we resolve forces exactly how we would anyway, taking each particle separately.

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Example 1: Yo-yo System

Back in Question 1 in the Forces section, we had two balls attached by taut string, suspended by a smooth peg.

We said that Ball 22 has twice the mass of Ball 11. Given that Ball 11 has a mass of 60 g60text{ g} and starts 30 cm30text{ cm} below the peg, calculate the tension in the string and the time taken for Ball 11 to reach the peg.

[4 marks]

Resolving for Ball 11:

T(0.06×9.8)=T0.588=0.06aT – (0.06 times 9.8) = T – 0.588 = 0.06a

Resolving for Ball 22:

(0.12×9.8)T=1.176T=0.12a(0.12 times 9.8) – T = 1.176 – T = 0.12a

From here, we have

0.12a=2T1.176=1.176T0.12a = 2T – 1.176 = 1.176 – T

which can be rearranged to

3T=2.3523T = 2.352, or T=0.784 NT = 0.784text{ N}

Substituting this back into one of our equations, we have 1.1760.784=0.12a1.176 – 0.784 = 0.12a, meaning that Ball 22 has a downward acceleration of a=3.27  ms2a = 3.27text{  ms}^{-2}. This means that Ball 11 accelerates towards the peg at 3.27  ms2 (to 2 dp)3.27text{  ms}^{-2} text{ (to }2text{ dp)}.

Using SUVAT, s=ut+12at2s = ut + dfrac{1}{2}at^2 gives

0.3=12×3.27×t20.3 = dfrac{1}{2} times 3.27 times t^2, so t=0.43 secondst = 0.43text{ seconds}

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Example 2: Rough Planes

Now, imagine a system of two weights attached by a thin piece of taut rope, both of mass 4 kg4text{ kg}. Weight Atext{A} is rested on a rough table with a coefficient of 0.20.2, and weight Btext{B} is suspended below a smooth pulley. What is the acceleration of both weights? What is the tension in the rope?

[5 marks]

Weight Atext{A} (vertical):

R=mg=4×9.8=39.2 NR = mg = 4 times 9.8 = 39.2text{ N}

Weight Atext{A} (horizontal):

TμR=maT – mu R = ma, giving T(0.2×39.2)=T7.84=4aT – (0.2 times 39.2) = T – 7.84 = 4a

Weight Btext{B} (vertical):

mgT=mamg – T = ma, giving 39.2T=4a39.2 – T = 4a

Therefore,

4a=39.2T=T7.844a = 39.2 – T = T – 7.84

which can be rearranged to

2T=47.042T = 47.04, or T=23.52 NT = 23.52text{ N}

Substituting back into one of our equations, we have 23.527.84=4a23.52 – 7.84 = 4a

giving

a=23.527.844=3.92  ms2a = dfrac{23.52 – 7.84}{4} = 3.92text{  ms}^{-2}

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Example 3: Rough Inclined Planes

Here’s another system of two weights attached by a thin piece of taut rope. Weight Atext{A}, of mass 9 kg9text{ kg}, is now on an inclined plane at an angle of 45°45° with a coefficient of 0.10.1, and weight Btext{B}, of mass 3 kg3text{ kg} is suspended below a smooth pulley. Does weight Btext{B} rise or fall? What is the rate of acceleration of both weights? What is the tension in the rope?

[7 marks]

Weight Atext{A} (perpendicular to motion):

R=mgcos45°=(9×9.8)cos45°=88.22R = mgcos 45° = (9 times 9.8)cos 45° = dfrac{88.2}{sqrt{2}}

Weight Atext{A} (parallel to motion, down slope):

mgsin45°TF=mgsin45°TμR=mamgsin 45° – T – F = mgsin 45° – T – mu R = ma

giving

(9×9.8)sin45°T(0.1×88.22)(9 times 9.8)sin 45° – T – left( 0.1 times dfrac{88.2}{sqrt{2}}right)

=88.22T8.822=9a= dfrac{88.2}{sqrt{2}} – T – dfrac{8.82}{sqrt{2}} = 9a.

Weight Btext{B} (upwards):

Tmg=maT – mg = ma, giving T(3×9.8)=3aT – (3 times 9.8) = 3a

or

T29.4=3aT – 29.4 = 3a

Equating the two equations:

9a=3T88.2=79.382T9a = 3T – 88.2 = dfrac{79.38}{sqrt{2}} – T

So

4T=79.382+88.2=144.334T = dfrac{79.38}{sqrt{2}} + 88.2 = 144.33

giving

T=36.08 N(to 2 dp)T = 36.08text{ N(to }2text{ dp)}

Therefore, we have

9a=(3×36.08)88.29a = (3 times 36.08) – 88.2

so

a=2.23  ms2a = 2.23text{  ms}^{-2}

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Connected Particles Example Questions

Question 1: We have two balls attached by taut string, suspended by a smooth peg.

If Ball Atext{A} has mass 100 g100text{ g} and Ball Btext{B} has mass 80 g80text{ g}, calculate the tension in the string and the acceleration of Ball Atext{A}.

[4 marks]

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Note: Here, “0.1g0.1g” is not the same as 0.1 grams0.1text{ grams}, it is 0.1 kg0.1text{ kg} by the acceleration due to gravity, gg. The same rule applies for 0.08g0.08g.

 

Resolving Ball Atext{A}:

(0.1×9.8)T=0.1a(0.1 times 9.8) – T = 0.1a

Resolving Ball Btext{B}:

T(0.08×9.8)=0.08aT – (0.08 times 9.8) = 0.08a

Therefore, we have

a=9.810T=12.5T9.8a = 9.8 – 10T = 12.5T – 9.8

So

22.5T=19.622.5T = 19.6

giving

T=0.871 N (to 3 dp)T = 0.871text{ N (to }3text{ dp)}

By extension, a=1.088  ms2 (to 3 dp)a = 1.088text{  ms}^{-2}text{ (to } 3text{ dp)}

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Question 2: For two bricks of mass 4 kg4text{ kg} linked by a rope on a smooth pulley, find the tension in the rope. Assume that the surface that brick Atext{A} has a coefficient of friction of 0.70.7.

[3 marks]

 

 

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Brick Atext{A} (vertical):

R=4×9.8=39.2 NR = 4 times 9.8 = 39.2text{ N}

Brick Atext{A} (horizontal):

TμR=maT – mu R = ma

gives

T(0.7×39.2)=4aT – (0.7 times 39.2) = 4a

Brick Btext{B} (vertical):

(4×9.8)T=4a(4 times 9.8) – T = 4a

So

T27.44=39.2TT – 27.44 = 39.2 – T

meaning

T=33.32 NT = 33.32text{ N}

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Question 3: A truck on a flat surface is towing a car up a hill with an incline of 30°30°. Given that the truck weighs 2000 kg2000text{ kg}, and the car weighs 1000 kg1000text{ kg} and is exerting a thrust of 2500 N2500 text{ N}, what thrust is required by the truck to pull the car up the hill with an acceleration of 1 ms21text{ ms}^{-2}?

Assume the coefficient of friction of both the hill and the flat surface are 0.250.25.

[7 marks]

 

 

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Resolving truck (vertically):

R=2000×9.8=19600 NR = 2000 times 9.8 = 19600text{ N}

Resolving truck (horizontally):

ThrustT(0.25×19600)=2000text{Thrust} – T – (0.25 times 19600) = 2000

Resolving car (perpendicular to F):

(1000×9.8)cos30°=8487=R(1000 times 9.8)cos 30° = 8487 = R

Resolving car (parallel to F):

2500+T(0.25×8487)(1000×9.8)sin30°=10002500 + T – (0.25 times 8487) – (1000 times 9.8)sin 30° = 1000

 

From the last equation, we have

T=1000+4900+21222500=5522 NT = 1000 + 4900 + 2122 – 2500 = 5522text{ N}

Back to the truck:

 Thrust55224900=2000text{ Thrust} – 5522 – 4900 = 2000

which gives

Thrust=12422 Ntext{Thrust} = 12422text{ N}

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Additional Resources

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Exam Tips Cheat Sheet

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Formula Booklet

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Specification Points Covered

R4 – Understand and use Newton’s third law; equilibrium of forces on a particle and motion in a straight line (restricted to forces in two perpendicular directions or simple cases of forces given as 2-D vectors); application to problems involving smooth pulleys and connected particles; resolving forces in 2 dimensions; equilibrium of a particle under coplanar forces
R5 – Understand and use addition of forces; resultant forces; dynamics for motion in a plane

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