Applied Physics Lab Report 1, Study Guides, Projects, Research of Physics

Lab Report 1 of Applied Physics. Topics covered are: Error Analysis. All the necessary calculations are done.

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2019/2020

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Lab Report No.1
Error Analysis
Applied Physics Instructor: Miss Fatima Mahjabeen
Miss Sundas Gul
Submitted by(Group 2):
Zain Mushtaq(287200)
M Ahmed Mushtaq(283632)
Mohammad Anas(290831)
Ghulam Mohayu Din(294071)
Mohammad Mahyar Ali(288484)
SEECS
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Lab Report No.

Error Analysis

Applied Physics Instructor: Miss Fatima Mahjabeen

Miss Sundas Gul

Submitted by(Group 2):

Zain Mushtaq(287200)

M Ahmed Mushtaq(283632)

Mohammad Anas(290831)

Ghulam Mohayu Din(294071)

Mohammad Mahyar Ali(288484)

SEECS

Abstract:

 Perimeter and Area

In this experiment, we find the perimeter and area of a

register and also calculate the standard error in

perimeter and area.

 To find the value of g

In this experiment, we find the value of g & calculate

standard error in g and percentage error in g by using a

simple pendulum.

theoretical distribution of a large population of such

estimates.

Standard error=

σ ´ x

s

n

Errors and their Types:

Error:

Error is defined as the difference between a

measured value and the expected value.

Types of Errors:

There are two types of errors:

 Random error

 Systematic error

Random error:

Random errors are statistical fluctuations in the

measured data due to the precision limitations of

the measurement device.Random errors can be

evaluated by statistical analysis and can be reduced

by averaging over a large number of obsrevations.

Systematic error:

Systematic errors are reproducible inaccuracies

that are consistently in the same direction.These

errors are difficult to detect and cannot be analyzed

by statistically.If a systematic error is identified

when calibrating against a standard,applying a

correction or a correction factor to compensate for

the effect can reduce the bias.Unlike random

errors,systematic errors cannot be detected or

reduced by increasing the number of observations.

Standard deviation in length = (S.D)

L

=

Σ ( L −

L )

2

N − 1

Standard deviation in width = (S.D)

W

=

Σ ( W −

W )

2

N − 1

5. We calculated the standard error in length and

width by using the following formulas:

Standard deviation in length= (S.E)

L

=

( S. D )

L

2

N

Standard deviation in width= (S.E)

W

=

( S. D )

W

2

N

6. We calculated the standard error in

perimeter[(S.E)

P

] and area[(S.E)

A

] of the register by

using the following formulas:

(S.E)

P

=

(

∂ P

∂ L

)

2

( S. E )

L

2

(

∂ P

∂W

)

2

( S. E )

W

2

(S.E)

A

=

(

∂ A

∂ L

)

2

( S. E )

L

2

(

∂ A

∂ W

)

2

( S. E )

W

2

Calculations:

Length

(cm)

Width

(cm)

Deviation

in length

L

o

= L −

L

Deviation

in width

W

o

= W −

W

(cm) (cm)

27.3 21.6 -0.08 -0.

27.4 21.7 0.02 0.

27.3 21.8 -0.08 0.

27.5 21.6 0.12 -0.

L =27.

W =21.

( S. D )

L

Σ ( L −

L )

2

N − 1

2

+(0.02)

2

+(−0.08)

2

+(0.12)

2

¿ √0.

¿ 0.096 cm

( S. D )

W

2

+(0.02)

2

+(0.12)

2

+(−0.08)

2

¿ (^) √0.0092=0.096 cm

( S. E )

L

( S. D )

L

2

N

2

=√0.

¿ 0.048 cm

( S. E )

W

( S. D )

W

2

N

2

=√0.

¿ 0.048 cm

Standard error in Parameter:

Experiment No.

Error analysis technique for finding the value

of “g” using a simple pendulum.

Procedure:

1. We measured the length of the string from it’s

one end to the middle of the metal bob.We took 3

readings and calculated the mean length

L

.

2. Now,we attached the string to an iron stand and

measured the time ‘t’ for 10 vibrations/oscillations

of the simple pendulum.Then,we calculated the

time period ‘T’ for one oscillation by:

T =

t

We calculated the mean time

T

.

3. We calculated the deviation in length:

L

o

= L −

L

And deviation in time:

T

o

= T −

T

4. We calculated the standard deviation in length

and time by using the following formulas:

Standard deviation in length= (S.D)

L

=

Σ ( L −

L )

2

N − 1

Standard deviation in time= (S.D)

T

=

Σ ( T −

T )

2

N − 1

(s) (cm) (s)

44.0 14.34 1.434 0.1 0.

43.9 12.57 1.257 0 -0.

43.8 13.69 1.369 -0.1 0.

L =¿

T =1.

( S. D )

L

Σ ( L −

L )

2

N − 1

2

+( 0 )

2

  • (−0.1)

2

=√0.01=0.

( S. D )

L

=0.1 cm

( S. D )

T

Σ ( T −

T )

2

N − 1

2

+(−0.096 )

2

  • ( 0.016)

2

¿ √0.

¿ 0.282 s

( S. E )

L

( S. D )

L

2

N

=√0.003=0.0578 cm

( S. E )

T

( S. D )

T

2

N

=√0.026=0.163 s

∂ g

∂T

∂ T

(

4 π

2

l

T

2 )

= 4 π

2

l T

− 3

(− 2 ) =− 8 π

2

l T

− 3

¿− 8 π

2

( (^) 43.9) ( (^) 1.35) (^) =1399.

∂ g

∂ L

4 π

2

T

2

4 π

2

2

( S. E )

g

( S. E )

L

2

(

∂ g

∂ L

)

2

+( S. E )

T

2

(

∂ g

∂T

)

2

¿ (^) √( 0.058)

2

2

2

2

¿ (^) √50,

¿ 223.84 cm s

− 2

g =

4 π

2

l

T

2

± (^ S. E )

g

g =(^ 946.58 ± 223.84 )^ cm s

− 2

Percentage error in ‘g’’:

% error =

(

)

× 100

The negative sign indicates that the measured value

is less than the actual value.

Conclusion:

The value of ‘g’ calculated by simple pendulum is:

g =(^ 946.58 ± 223.84 )^ cm s

− 2