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ticker tape timer

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ticker tape timer
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posted:
11/25/2011
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The motion of a trolley moving along a straight runway is studied.



A paper tape is attached to the tail of the trolley



The paper tape passes through a ticker tape timer

Ticker

The timer prints dots on the tape at regular time intervals Tape

Timer









Trolley Paper tape

attached to the

trolley

As the trolley moves, the paper passes under through the timer

and dots are printed at regular time intervals on the tape.





Ticker

Tape

Timer









Dot printed by the

ticker tape timer on

the paper tape

Dots are printed on the tape with fixed time intervals Dt.







If the trolley is moving with uniform velocity, the dots

are evenly spaced.

Dots are printed on the tape with fixed time intervals Dt.







If the trolley is moving with increasing speed, the

spacing of the dots increases.









first dot last dot

Dots are printed on the tape with fixed time intervals Dt.







If the trolley is moving with decreasing speed, the

spacing of the dots decreases.









first dot last dot

The frequency of the ticker tape timer = fs



fs is the number of dots that the timer prints in one second.



fs is measured in Hz (Hertz).



If fs = 50 Hz , 50 dots are printed in 1 s.



If fs = 100 Hz , 100 dots are printed in 1 s.

The time interval Dt between printing two adjacent dots

is given by

1

Dt 

fs

If fs is in Hz, Dt is in s.



If fs = 50 Hz , Dt = 0.02 s.

One dot is printed every 0.02 s.



If fs = 100 Hz , Dt = 0.01 s.

One dot is printed every 0.01 s.

The time interval between printing two adjacent dots is

also known as a ‘tick’.



For a ticker tape timer of 50 Hz,



a one-tick interval is 0.02 s ,



a two-tick interval is 0.04 s ,



a three-tick interval is 0.06 s ,



a five-tick interval is 0.1 s .

The time interval between printing two adjacent dots is

also known as a ‘tick’.



For a ticker tape timer of 100 Hz,



a one-tick interval is 0.01 s ,



a two-tick interval is 0.02 s ,



a three-tick interval is 0.03 s ,



a five-tick interval is 0.05 s .

A tape can be analyzed in one-tick intervals.

A section of the tape is selected for analysis.

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3

first dot last dot



The instant when the first dot is printed is assigned t = 0.



The instant when the second dot is printed is assigned t = Dt.

The instant when the third dot is printed is assigned t = 2Dt.



The instant when the fourth dot is printed is assigned t = 3Dt.

A tape can be analyzed in one-tick intervals.

A section of the tape is selected for analysis.

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3





The distance travelled by the object is l1 from t = 0 to t = Dt

l1

The average velocity in this time interval is V1 

Dt

V1 can be assumed to be the instantaneous velocity of the object at

the instant t = 0.5 Dt

A tape can be analyzed in one-tick intervals.

A section of the tape is selected for analysis.

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3





The distance travelled by the object is l2 from t = Dt to t =2Dt

l2

The average velocity in this time interval is V2 

Dt

V2 can be assumed to be the instantaneous velocity of the object at

the instant t = 1.5 Dt

A tape can be analyzed in one-tick intervals.

A section of the tape is selected for analysis.

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3





The distance travelled by the object is l3 from t = 2Dt to t =3Dt

l3

The average velocity in this time interval is V3 

Dt

V3 can be assumed to be the instantaneous velocity of the object at

the instant t = 2.5 Dt

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3



A velocity-time graph is now available.

time velocity Velocity



t1 = 0.5 Dt V1 = l1Dt

t2 = 1.5 Dt V2 = l2Dt V3

t3 = 2.5 Dt V3 = l3Dt V2



Note that V1

V1 : V2 : V3 = l1 : l2 : l3 Time

0 Dt Dt Dt

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3



time velocity The average acceleration of the object

t1 = 0.5 Dt V1 = l1Dt in the interval t1 < t < t2 is given by

t2 = 1.5 Dt V2 = l2Dt

V2  V1

t3 = 2.5 Dt V3 = l3Dt a12 

t 2  t1

l 2 l1



 Dt Dt

1.5Dt  0.5Dt



l 2  l1



(Dt ) 2

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3



time velocity The average acceleration of the object

t1 = 0.5 Dt V1 = l1Dt in the interval t2 < t < t3 is given by

t2 = 1.5 Dt V2 = l2Dt

V3  V2

t3 = 2.5 Dt V3 = l3Dt a23 

t3  t 2

l3 l 2



 Dt Dt

2.5Dt  1.5Dt



l3  l 2



(Dt ) 2

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3

If the object is moving with uniform acceleration, the velocity-

time graph is a straight line.



Velocity

V3  V2 = V2 – V1



l3 - l2 = l2 – l1 V3

V2

V1 ,V2 , V3 form an

V1

arithmetic progression and

so do l1 ,l2 , l3 Time

0 Dt Dt Dt

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3

If the object is moving with uniform acceleration, the velocity-

time graph is a straight line.



a12 = a23 Velocity







l2  l1 l3  l 2 V3



(Dt ) 2 (Dt ) 2 V2



V1



Time

0 Dt Dt Dt

t=0 t=Dt t=2Dt t=3Dt







l1 l2 l3

If the object is moving with uniform acceleration, the velocity-

time graph is a straight line.

The uniform acceleration

is also given by Velocity



V3  V1

a

t 3  t1 V3

l3 l 2

 V2

 D t Dt

2 .5 Dt  0 .5 Dt V1



l3  l1 Time

 0 Dt Dt Dt

2( Dt ) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 50 Hz. The time interval for one tick is

0.02 s









first dot 8 mm 11 mm 14 mm 17 mm

last dot

The sequence has a common difference

of 3 mm. Therefore the object is

moving with uniform acceleration.



0.011 m 0.008 m



a 0.02 s 0.02 s  0.011 m  0.008 m  7.5 m s - 2

0.03 s  0.01 s (0.02 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 50 Hz. The time interval for one tick is

0.02 s









first dot 8 mm 11 mm 14 mm 17 mm

last dot

The sequence has a common difference

of 3 mm. Therefore the object is

moving with uniform acceleration.



0.017 m 0.014 m



a 0.02 s 0.02 s  0.017 m  0.014 m  7.5 m s - 2

0.07 s  0.05 s (0.02 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 50 Hz. The time interval for one tick is

0.02 s









first dot 8 mm 11 mm 14 mm 17 mm

last dot

The sequence has a common difference

of 3 mm. Therefore the object is

moving with uniform acceleration.



0.017 m 0.011 m



a 0.02 s 0.02 s  0.017 m  0.011 m  7.5 m s - 2

0.07 s  0.03 s 2(0.02 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 50 Hz. The time interval for one tick is

0.02 s









first dot 8 mm 11 mm 14 mm 17 mm

last dot

The sequence has a common difference

of 3 mm. Therefore the object is

moving with uniform acceleration.



0.017 m 0.008 m



a 0.02 s 0.02 s  0.017 m  0.008 m  7.5 m s - 2

0.07 s  0.01 s 3(0.02 s) 2

Very often, a ticker tape is analyzed in intervals longer

than one tick. This is because





• the length is very short for one tick. There is

large percentage error in measuring the length

corresponding to one tick.

• the spacing between the dots may vary in an

irregular pattern. The reason may be that the

timer does not print the dots in exactly the same

time interval. Analyzing the paper tape at

intervals of more than one tick may help to

averaging the errors.

A tape can be analyzed in five-tick intervals.

The time interval for one-tick is Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3



The instant when the first dot is printed is assigned t = 0.

The instant when the sixth dot is printed is assigned t = 5Dt.

The instant when the eleventh dot is printed is assigned t = 10Dt.

The instant when the sixteenth dot is printed is assigned t = 15Dt.

A tape can be analyzed in five-tick intervals.

The time interval for one-tick is Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The distance travelled by the object is l1 from t = 0 to t = 5Dt

l1

The average velocity in this time interval is V1 

5Dt

V1 can be assumed to be the instantaneous velocity of the object at

the instant t = 2.5 Dt

A tape can be analyzed in five-tick intervals.

The time interval for one-tick is Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The distance travelled by the object is l2 from t = 5Dt to t = 10Dt

l2

The average velocity in this time interval is V2 

5Dt

V2 can be assumed to be the instantaneous velocity of the object at

the instant t = 7.5 Dt

A tape can be analyzed in five-tick intervals.

The time interval for one-tick is Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The distance travelled by the object is l3 from t = 10Dt to t = 15Dt

l3

The average velocity in this time interval is V3 

5Dt

V3 can be assumed to be the instantaneous velocity of the object at

the instant t = 12.5 Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

A velocity-time graph is now available.

Velocity

time velocity

t1 = 2.5 Dt V1 = l1Dt

t2 = 7.5 Dt V2 = l2Dt V3

t3 = 12.5 Dt V3 = l3Dt V2



Note that V1



V1 : V2 : V3 = l1 : l2 : l3 Time

0 Dt Dt Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The average acceleration of the object

time velocity

in the interval t1 < t < t2 is given by

t1 = 2.5 Dt V1 = l1Dt

t2 = 7.5 Dt V2 = l2Dt V2  V1

a12 

t 2  t1

t3 = 12.5 Dt V3 = l3Dt

l2 l1



 5 Dt 5Dt

7.5Dt  2.5Dt



l 2  l1



(5Dt ) 2

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The average acceleration of the object

time velocity

in the interval t2 < t < t3 is given by

t1 = 2.5 Dt V1 = l1Dt

t2 = 7.5 Dt V2 = l2Dt V3  V2

a23 

t3  t 2

t3 = 12.5 Dt V3 = l3Dt

l3 l2



 5Dt 5Dt

12.5Dt  7.5Dt



l3  l 2



(5Dt ) 2

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

If the object is moving with uniform acceleration, the velocity-

time graph is a straight line.

Velocity

V3  V2 = V2 – V1



l3 - l2 = l2 – l1 V3

V2

V1 ,V2 , V3 form an

arithmetic progression and V1

so do l1 ,l2 , l3

Time

0 Dt Dt Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

If the object is moving with uniform acceleration, the velocity-

time graph is a straight line.

Velocity



a12 = a23

V3

l 2  l1 l3  l 2 V2



(5Dt ) 2 (5Dt ) 2

V1



Time

0 Dt Dt Dt

t=0 t=5Dt t=10Dt t=15Dt







first dot last dot

l1 l2 l3

The uniform acceleration is also

given by Velocity

V3  V1

a

t3  t1

V3

l3 l2



 5Dt 5Dt

V2

12.5Dt  2.5Dt

V1

l3  l1

 Time

2(5Dt ) 2 0 Dt Dt Dt

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 100 Hz. The time interval for one tick is

0.01 s









first dot 28 mm 34 mm 40 mm 46 mm last dot

The sequence has a common difference

of 6 mm. Therefore the object is

moving with uniform acceleration.



0.034 m 0.028 m



a 0.05 s 0.05 s  0.034 m  0.028 m  2.4 m s - 2

0.075 s  0.025 s (0.05 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 100 Hz. The time interval for one tick is

0.01 s









first dot 28 mm 34 mm 40 mm 46 mm last dot

The sequence has a common difference

of 6 mm. Therefore the object is

moving with uniform acceleration.



0.046 m 0.040 m



a 0.05 s 0.05 s  0.046 m  0.040 m  2.4 m s - 2

0.175 s  0.125 s (0.05 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 100 Hz. The time interval for one tick is

0.01 s









first dot 28 mm 34 mm 40 mm 46 mm last dot

The sequence has a common difference

of 6 mm. Therefore the object is

moving with uniform acceleration.



0.046 m 0.034 m



a 0.05 s 0.05 s  0.046 m  0.034 m  2.4 m s - 2

0.175 s  0.075 s 2(0.05 s) 2

Consider the section of the paper tape below, printed by a ticker

tape timer of frequency 100 Hz. The time interval for one tick is

0.01 s









first dot 28 mm 34 mm 40 mm 46 mm last dot

The sequence has a common difference

of 6 mm. Therefore the object is

moving with uniform acceleration.



0.046 m 0.028 m



a 0.05 s 0.05 s  0.046 m  0.028 m  2.4 m s - 2

0.175 s  0.025 s 3(0.05 s) 2

The disadvantages of using a ticker tape timer are



• The timer prints dots by hammering on the tape. As a

result the object experiences a frictional force which

opposes its motion. The motion of the object is affected.

For good results, the timer has to be adjusted so that the

hammering force on the tape has to be minimized but a

weak hammering force will print dots which are not

clear enough.

• The timer can only study the motion of an object moving

along a straight line in one direction only. The method

fails if the object reverses its direction of motion.


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