Experiment-4 Mass Moment of Inertia - Copy

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  • 7/24/2019 Experiment-4 Mass Moment of Inertia - Copy

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    Experiment 4: Mass Moment of Inertia I

    Experimental Mass Moment of Inertia Part A

    Equipment:Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "

    lenths of steel wire#

    Objectives:1# $he experiment is to determine experimentall% the moment of

    inertia and radi!s of %ration of a rectan!lar &ar#

    2# 'omparison &etween experimental and theoretical res!lts#

    Experimental procedure:

    1# $he (al!es of lenth of rope, L, centre distance, r, mass ofrectan!lar &ar, M, and the dimensions of &ar a, &, and l are

    o&tained and meas!red#

    2# $he &ar is connected with e%e &olts with nelii&le mass onto the

    wires with the clips pro(ided#

    "# $he &ar is twisted hori)ontall% to p!t it into oscillation a&o!t its

    (ertical axis to a simple harmonic motion#

    4# $he &ar is left !ntil it oscillates in a stead% state#

    *# $he time is o&tained in seconds ta+en for 20 oscillations#

    # $he (al!e is di(ided with the n!m&er of oscillations to o&tain timeta+en for 1 oscillation# $he experiment is repeated to o&tain time

    ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise

    (al!e for the period in seconds#

    # $he (al!e of the radi!s of %ration, ., and moment of inertia, I are

    calc!lated !sin the followin e/!ation pro(ided#

    t=2( IL

    Mg r2 ) or t=2(

    k2L

    r2

    g) for I=M k2

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    Experiment 4: Mass Moment of Inertia I

    ResultsMass of rectan!lar &ar: 1#+

    Item Lengt !m"a 0#02*& 0#04l 0#202L 1#0r 0#0**

    $a&le 4#1: imensions

    $a&le 4#2: With afacing up,

    Oscillation Period !s" #ime for $oscillation !s"

    20 41 2#0*"0 2 2#040 82 2#0**0 10" 2#00 12* 2#08

    Average time for $ oscillation !s" %&'(

    $a&le 4#": ithb

    facin !p,Oscillation Period !s" #ime for $

    oscillation !s"20 42 2#1"0 " 2#140 84 2#1*0 10 2#120 12 2#12

    Average time for $ oscillation !s" %&$$

    )iscussions$heoretical (al!e for the moment of inertia of a rectan!lar &ar is,

    I=M(a2+l2 )

    12or I=

    M(a2+b2 )12

    With afacing up experimental calculation theoretical calculation * error

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    Experiment 4: Mass Moment of Inertia I

    t=2( IL

    Mg r2 ) I=M(a

    2+l

    2 )12

    I I=0.00558kg.m2 I=0.00552kg.m2 1#0

    With afacing up

    experimental calculation

    K= I

    M

    theoretical calculation

    K= I

    M

    * error

    K K= 0.0591m2

    K= 0.0587m2

    0#8

    With bfacing up

    experimental calculation

    t=2

    ( IL

    Mg r2 )

    theoretical calculation

    I=M(a2+l2 )

    12 * error

    I I=0.00585kg.m2

    I=0.00565 kg.m2

    "#*4

    With bfacing up

    experimental calculation

    K= I

    M

    theoretical calculation

    K= I

    M

    * error

    K K= 0.0605m2

    K=0.0594 m2

    1#8*

    +onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and

    moment of inertia 3I were compared with theoretical (al!es o&tained

    !sin the form!la pro(ided# $he error fo!nd in the experiment is less than

    *5 in each case with a facin !p and & facin !p# $herefore the

    experiment data is accepted# $he main reason for occ!rrence of error is

    d!e to the h!man error that occ!r in the process of record the time withrespect to start and stoppin of stopwatch# In concl!sion it is pro(ed that

    &oth the form!la we !sed in experimental and theoretical calc!lation is

    accepted to !se#

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    Experiment 4: Mass Moment of Inertia I

    Experimental Mass Moment of Inertia Part ,

    Equipment:

    Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "

    lenths of steel wire#

    Objectives:1# $he experiment is to determine experimentall% the moment of

    inertia and radi!s of %ration of a rin#

    2# 'omparison &etween experimental and theoretical res!lts#

    Experimental procedure:

    1# $he (al!es of lenth of rope, L, mean radi!s of rin, 6, o!ter radi!s

    r1 , inner radi!s, r2 , and mass of rin, M are o&tained and

    meas!red#2# $he rin is connected with e%e &olts with nelii&le mass onto the

    wires with the clips pro(ided#"# $he rin is twisted hori)ontall% to p!t it into oscillation a&o!t its

    (ertical axis to a simple harmonic motion#4# $he rin is left !ntil it oscillates in a stead% state#

    *# $he time is o&tained in seconds ta+en for 20 oscillations#

    # $he (al!e is di(ided with the n!m&er of oscillations to o&tain time

    ta+en for 1 oscillation# $he experiment is repeated to o&tain time

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    Experiment 4: Mass Moment of Inertia I

    ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise

    (al!e for the period in seconds#

    # $he (al!e of the radi!s of %ration, ., and moment of inertia, I are

    calc!lated !sin the followin e/!ation pro(ided#

    t=2 ( ILMg r2 ) or t=2(k2L

    r2

    g) for I=M k2

    R=r1+r

    2

    2

    ResultsMass of rectan!lar &ar: 1#+

    Item Lengt !m"r1 0#08

    r2 0#0*

    l 0#024L 1#0

    $a&le: 6in imensions

    $a&le 4#4: With afacing up,

    Oscillation Period !s" #ime for $

    oscillation !s"20 41 2#0*"0 2 2#040 84 2#1*0 10* 2#10 12 2#1

    Average time for $ oscillation !s" %&'-

    )iscussions$heoretical (al!e for the moment of inertia of a rectan!lar &ar is,

    I=l (r1

    4r

    2

    4 )2

    =mass per unit volume , r1=outer radius , r2=inner radius

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    Experiment 4: Mass Moment of Inertia I

    experimental calculation theoretical calculation * error

    R=r1+r

    2

    2

    67 0#08

    v= r12

    l r22

    ( 70.000246

    m

    3

    =M

    v

    =7967.48 kg /m3

    sin the form!la,

    t=2

    ( IL

    Mg r2

    )and sol(in for I,

    I=0.00974kg.m2

    sin the form!la,

    I=l (r1

    4r

    2

    4 )

    2

    and sol(in for I,

    I=0.00935 kg.m2

    4#1

    experimental calculation

    K= I

    M

    theoretical calculation

    K= I

    M

    * error

    K= 0.0705m2 K= 0.0691m2 2#0"

    +onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and

    moment of inertia 3I were compared with theoretical (al!es o&tained

    !sin the form!la pro(ided# $he error fo!nd in the experiment is less than

    *5 in each case with a facin !p and & facin !p# $herefore the

    experiment data is accepted# $he main reason for occ!rrence of error is

    d!e to the h!man error that occ!r in the process of record the time withrespect to start and stoppin of stopwatch# In concl!sion it is pro(ed that

    &oth the form!la we !sed in experimental and theoretical calc!lation is

    accepted to !se#

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    Experiment 4: Mass Moment of Inertia I

    Experimental Mass Moment of Inertia Part +

    Equipment:Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "

    lenths of steel wire#

    Objectives:1# $he experiment is to determine experimentall% the moment of

    inertia and radi!s of %ration of a c%linder#

    2# 'omparison &etween experimental and theoretical res!lts#

    Experimental procedure:

    1# $he (al!es of lenth of rope, L, center distance of c%linder, r, mass

    of c%linder, M, lenth of c%linder, l, and radi!s of c%linder, 6, are

    o&tain and meas!re#

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    Experiment 4: Mass Moment of Inertia I

    2# $he c%linder is connected with e%e &olts with nelii&le mass onto

    the wires with the clips pro(ided#"# $he c%linder is twisted hori)ontall% to p!t it into oscillation a&o!t its

    (ertical axis to a simple harmonic motion#4# $he c%linder is left !ntil it oscillates in a stead% state#

    *# $he time is o&tained in seconds ta+en for 20 oscillations#

    # $he (al!e is di(ided with the n!m&er of oscillations to o&tain time

    ta+en for 1 oscillation# $he experiment is repeated to o&tain time

    ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise

    (al!e for the period in seconds#

    # $he (al!e of the radi!s of %ration, ., and moment of inertia, I are

    calc!lated !sin the followin e/!ation pro(ided#

    t=2

    ( IL

    Mg r2

    )or t=2

    (k2L

    r2

    g)for I=M k

    2

    ResultsMass of rectan!lar &ar: 4#8 +

    Item Lengt !m"R 0#0*

    r 0#0*

    l 0#0"L 1#0

    $a&le: 6in imensions

    $a&le 4#4: With afacing up,

    Oscillation Period !s" #ime for $

    oscillation !s"20 "4 1#"0 *1 1#40 8 1#*0 8 1#20 10" 1#2

    Average time for $ oscillation !s" $&.$

    )iscussionsTheoretical value for the moment of inertia of a rectangular bar is,

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    Experiment 4: Mass Moment of Inertia I

    I=M R

    2

    2

    M = Mass of cylinder, R= radius of cylinder

    experimental calculation theoretical calculation * error

    sin the form!la,

    t=2( IL

    Mg r2 )

    and sol(in for I,

    I=0.0158 kg.m2

    sin the form!la,

    I=M R

    2

    2

    and sol(in for I,

    I=0.0151 kg.m2

    4#4

    experimental calculation

    K= I

    M

    theoretical calculation

    K= I

    M* error

    K= 0.0576m2

    K= 0.0563m2

    2#"1

    +onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and

    moment of inertia 3I were compared with theoretical (al!es o&tained

    !sin the form!la pro(ided# $he error fo!nd in the experiment is less than

    *5 in each case with a facin !p and & facin !p# $herefore the

    experiment data is accepted# $he main reason for occ!rrence of error is

    d!e to the h!man error that occ!r in the process of record the time with

    respect to start and stoppin of stopwatch# In concl!sion it is pro(ed that

    &oth the form!la we !sed in experimental and theoretical calc!lation is

    accepted to !se#