Calculating extensions in elastic string
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Could anyone please help me with the following question?
Here's my failed line of reasoning so far:
My diagram:
You can see that I am assuming that P moves down to lie vertically under it's original position, is even this correct?
Otherwise:
I've tried a few ways, here's the most naive, thanks for any help:
Let extension in AP = $x_1$ and extension in PB be $x_2$ then:
$L_1=frac320,cos,theta$
and so
$x_1=frac320,cos,theta-frac320$
and
$L_2=frac120,sin,theta$
and so
$x_2=frac120,sin,theta-frac120$
Hence:
$fracx_1x_2=fracfrac60-60,cos,theta400,cos,thetafrac20-20,sin,theta400,sin,theta=frac60-60,cos,thetacosthetatimesfracsin,theta20-20,sin,theta$
which can be simplified to:
$frac(3-3,cos,theta),sin,theta(1-sin,theta),cos,theta$
Which isn't the required answer. Thanks for any help.
classical-mechanics
add a comment |Â
up vote
1
down vote
favorite
Could anyone please help me with the following question?
Here's my failed line of reasoning so far:
My diagram:
You can see that I am assuming that P moves down to lie vertically under it's original position, is even this correct?
Otherwise:
I've tried a few ways, here's the most naive, thanks for any help:
Let extension in AP = $x_1$ and extension in PB be $x_2$ then:
$L_1=frac320,cos,theta$
and so
$x_1=frac320,cos,theta-frac320$
and
$L_2=frac120,sin,theta$
and so
$x_2=frac120,sin,theta-frac120$
Hence:
$fracx_1x_2=fracfrac60-60,cos,theta400,cos,thetafrac20-20,sin,theta400,sin,theta=frac60-60,cos,thetacosthetatimesfracsin,theta20-20,sin,theta$
which can be simplified to:
$frac(3-3,cos,theta),sin,theta(1-sin,theta),cos,theta$
Which isn't the required answer. Thanks for any help.
classical-mechanics
It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58
add a comment |Â
up vote
1
down vote
favorite
up vote
1
down vote
favorite
Could anyone please help me with the following question?
Here's my failed line of reasoning so far:
My diagram:
You can see that I am assuming that P moves down to lie vertically under it's original position, is even this correct?
Otherwise:
I've tried a few ways, here's the most naive, thanks for any help:
Let extension in AP = $x_1$ and extension in PB be $x_2$ then:
$L_1=frac320,cos,theta$
and so
$x_1=frac320,cos,theta-frac320$
and
$L_2=frac120,sin,theta$
and so
$x_2=frac120,sin,theta-frac120$
Hence:
$fracx_1x_2=fracfrac60-60,cos,theta400,cos,thetafrac20-20,sin,theta400,sin,theta=frac60-60,cos,thetacosthetatimesfracsin,theta20-20,sin,theta$
which can be simplified to:
$frac(3-3,cos,theta),sin,theta(1-sin,theta),cos,theta$
Which isn't the required answer. Thanks for any help.
classical-mechanics
Could anyone please help me with the following question?
Here's my failed line of reasoning so far:
My diagram:
You can see that I am assuming that P moves down to lie vertically under it's original position, is even this correct?
Otherwise:
I've tried a few ways, here's the most naive, thanks for any help:
Let extension in AP = $x_1$ and extension in PB be $x_2$ then:
$L_1=frac320,cos,theta$
and so
$x_1=frac320,cos,theta-frac320$
and
$L_2=frac120,sin,theta$
and so
$x_2=frac120,sin,theta-frac120$
Hence:
$fracx_1x_2=fracfrac60-60,cos,theta400,cos,thetafrac20-20,sin,theta400,sin,theta=frac60-60,cos,thetacosthetatimesfracsin,theta20-20,sin,theta$
which can be simplified to:
$frac(3-3,cos,theta),sin,theta(1-sin,theta),cos,theta$
Which isn't the required answer. Thanks for any help.
classical-mechanics
asked Jul 16 at 10:51
gnitsuk
525
525
It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58
add a comment |Â
It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58
It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58
It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58
add a comment |Â
2 Answers
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0
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Well, here's my other attempt which does not assume that P moves down vertically:
I'll be using Hooke's law $T=fraclambda xa$
Let h = the height of the triangle in the diagram, i.e. the distance through which P falls.
$h=L_2,cos,theta=L_1,sin,theta$
and so
$L_1=fracL_2,cos,thetasin,theta$ - call this "Equation A"
$L_2=fracL_1,sin,thetacos,theta$ - call this "Equation B"
Resolving forces horizontally:
$T_1,cos,theta-T_2,sin,theta=0$ - Call this "Equation 1"
and Hooke's law gives us:
$T_1=fraclambda(L_1-frac320)frac320$
and
$T_2=fraclambda(L_2-frac120)frac120$
And so Eqaution 1 gives us:
$frac203lambda(L_1-frac320),cos,theta-20lambda(L_2-frac120),sin,theta=0$
Substituting fot $L_1$ from Equation A gives:
$lambda(frac203timesfracL_2,cos,thetasin,theta-1),cos,theta=lambda(20L_2-1),sin,theta$
Which rearranges to:
$L_2=frac3,sintheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Similarly substituting for $L_2$ from Equation B leads to:
$L_1=frac3,costheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Now we are asked to find $fracL_1 - frac320L_2-frac120$
Which is equal to:
$frac60,cos,theta(cos,theta-sin,theta)-3(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)/frac60,sintheta(cos,theta-sin,theta)-(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)$
Which simplifies to:
$frac9,sin^2theta-3,sin,theta,cos,theta3,sin,theta,cos,theta-cos^2theta$
Which is not the required answer.
add a comment |Â
up vote
0
down vote
We have
$$
|AP|_0 = 15\
|BP|_0 = 5\
r = frac_02\
|AP| = 2rcostheta\
|BP| = 2rsintheta
$$
then
$$
fracAPBP = frac20 cos (theta )-1520 sin (theta )-5 = frac4 cos (theta )-34 sin (theta )-1
$$
the solution follows as in
Calculation of the modulus of elasticity of a stretched string
NOTE
with $lambda$ the elastic modulus,
$$
lambdaleft(fracAPAPright)costheta = lambdaleft(fracBPright)sintheta
$$
(In equilibrium the horizontal projection for $F_AP$ and $F_PB$ are equal) then
$$
fracAPBP=fracsinthetacosthetafracAP
$$
or as expected
$$
frac4 cos theta-34 sintheta-1 = 3left(fracsinthetacosthetaright)
$$
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
add a comment |Â
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
0
down vote
Well, here's my other attempt which does not assume that P moves down vertically:
I'll be using Hooke's law $T=fraclambda xa$
Let h = the height of the triangle in the diagram, i.e. the distance through which P falls.
$h=L_2,cos,theta=L_1,sin,theta$
and so
$L_1=fracL_2,cos,thetasin,theta$ - call this "Equation A"
$L_2=fracL_1,sin,thetacos,theta$ - call this "Equation B"
Resolving forces horizontally:
$T_1,cos,theta-T_2,sin,theta=0$ - Call this "Equation 1"
and Hooke's law gives us:
$T_1=fraclambda(L_1-frac320)frac320$
and
$T_2=fraclambda(L_2-frac120)frac120$
And so Eqaution 1 gives us:
$frac203lambda(L_1-frac320),cos,theta-20lambda(L_2-frac120),sin,theta=0$
Substituting fot $L_1$ from Equation A gives:
$lambda(frac203timesfracL_2,cos,thetasin,theta-1),cos,theta=lambda(20L_2-1),sin,theta$
Which rearranges to:
$L_2=frac3,sintheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Similarly substituting for $L_2$ from Equation B leads to:
$L_1=frac3,costheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Now we are asked to find $fracL_1 - frac320L_2-frac120$
Which is equal to:
$frac60,cos,theta(cos,theta-sin,theta)-3(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)/frac60,sintheta(cos,theta-sin,theta)-(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)$
Which simplifies to:
$frac9,sin^2theta-3,sin,theta,cos,theta3,sin,theta,cos,theta-cos^2theta$
Which is not the required answer.
add a comment |Â
up vote
0
down vote
Well, here's my other attempt which does not assume that P moves down vertically:
I'll be using Hooke's law $T=fraclambda xa$
Let h = the height of the triangle in the diagram, i.e. the distance through which P falls.
$h=L_2,cos,theta=L_1,sin,theta$
and so
$L_1=fracL_2,cos,thetasin,theta$ - call this "Equation A"
$L_2=fracL_1,sin,thetacos,theta$ - call this "Equation B"
Resolving forces horizontally:
$T_1,cos,theta-T_2,sin,theta=0$ - Call this "Equation 1"
and Hooke's law gives us:
$T_1=fraclambda(L_1-frac320)frac320$
and
$T_2=fraclambda(L_2-frac120)frac120$
And so Eqaution 1 gives us:
$frac203lambda(L_1-frac320),cos,theta-20lambda(L_2-frac120),sin,theta=0$
Substituting fot $L_1$ from Equation A gives:
$lambda(frac203timesfracL_2,cos,thetasin,theta-1),cos,theta=lambda(20L_2-1),sin,theta$
Which rearranges to:
$L_2=frac3,sintheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Similarly substituting for $L_2$ from Equation B leads to:
$L_1=frac3,costheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Now we are asked to find $fracL_1 - frac320L_2-frac120$
Which is equal to:
$frac60,cos,theta(cos,theta-sin,theta)-3(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)/frac60,sintheta(cos,theta-sin,theta)-(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)$
Which simplifies to:
$frac9,sin^2theta-3,sin,theta,cos,theta3,sin,theta,cos,theta-cos^2theta$
Which is not the required answer.
add a comment |Â
up vote
0
down vote
up vote
0
down vote
Well, here's my other attempt which does not assume that P moves down vertically:
I'll be using Hooke's law $T=fraclambda xa$
Let h = the height of the triangle in the diagram, i.e. the distance through which P falls.
$h=L_2,cos,theta=L_1,sin,theta$
and so
$L_1=fracL_2,cos,thetasin,theta$ - call this "Equation A"
$L_2=fracL_1,sin,thetacos,theta$ - call this "Equation B"
Resolving forces horizontally:
$T_1,cos,theta-T_2,sin,theta=0$ - Call this "Equation 1"
and Hooke's law gives us:
$T_1=fraclambda(L_1-frac320)frac320$
and
$T_2=fraclambda(L_2-frac120)frac120$
And so Eqaution 1 gives us:
$frac203lambda(L_1-frac320),cos,theta-20lambda(L_2-frac120),sin,theta=0$
Substituting fot $L_1$ from Equation A gives:
$lambda(frac203timesfracL_2,cos,thetasin,theta-1),cos,theta=lambda(20L_2-1),sin,theta$
Which rearranges to:
$L_2=frac3,sintheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Similarly substituting for $L_2$ from Equation B leads to:
$L_1=frac3,costheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Now we are asked to find $fracL_1 - frac320L_2-frac120$
Which is equal to:
$frac60,cos,theta(cos,theta-sin,theta)-3(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)/frac60,sintheta(cos,theta-sin,theta)-(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)$
Which simplifies to:
$frac9,sin^2theta-3,sin,theta,cos,theta3,sin,theta,cos,theta-cos^2theta$
Which is not the required answer.
Well, here's my other attempt which does not assume that P moves down vertically:
I'll be using Hooke's law $T=fraclambda xa$
Let h = the height of the triangle in the diagram, i.e. the distance through which P falls.
$h=L_2,cos,theta=L_1,sin,theta$
and so
$L_1=fracL_2,cos,thetasin,theta$ - call this "Equation A"
$L_2=fracL_1,sin,thetacos,theta$ - call this "Equation B"
Resolving forces horizontally:
$T_1,cos,theta-T_2,sin,theta=0$ - Call this "Equation 1"
and Hooke's law gives us:
$T_1=fraclambda(L_1-frac320)frac320$
and
$T_2=fraclambda(L_2-frac120)frac120$
And so Eqaution 1 gives us:
$frac203lambda(L_1-frac320),cos,theta-20lambda(L_2-frac120),sin,theta=0$
Substituting fot $L_1$ from Equation A gives:
$lambda(frac203timesfracL_2,cos,thetasin,theta-1),cos,theta=lambda(20L_2-1),sin,theta$
Which rearranges to:
$L_2=frac3,sintheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Similarly substituting for $L_2$ from Equation B leads to:
$L_1=frac3,costheta(cos,theta-sin,theta)20,cos^2theta-60,sin^2theta$
Now we are asked to find $fracL_1 - frac320L_2-frac120$
Which is equal to:
$frac60,cos,theta(cos,theta-sin,theta)-3(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)/frac60,sintheta(cos,theta-sin,theta)-(20,cos^2theta-60,sin^2theta)20(cos^2theta-60,sin^2theta)$
Which simplifies to:
$frac9,sin^2theta-3,sin,theta,cos,theta3,sin,theta,cos,theta-cos^2theta$
Which is not the required answer.
answered Jul 16 at 14:15
gnitsuk
525
525
add a comment |Â
add a comment |Â
up vote
0
down vote
We have
$$
|AP|_0 = 15\
|BP|_0 = 5\
r = frac_02\
|AP| = 2rcostheta\
|BP| = 2rsintheta
$$
then
$$
fracAPBP = frac20 cos (theta )-1520 sin (theta )-5 = frac4 cos (theta )-34 sin (theta )-1
$$
the solution follows as in
Calculation of the modulus of elasticity of a stretched string
NOTE
with $lambda$ the elastic modulus,
$$
lambdaleft(fracAPAPright)costheta = lambdaleft(fracBPright)sintheta
$$
(In equilibrium the horizontal projection for $F_AP$ and $F_PB$ are equal) then
$$
fracAPBP=fracsinthetacosthetafracAP
$$
or as expected
$$
frac4 cos theta-34 sintheta-1 = 3left(fracsinthetacosthetaright)
$$
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
add a comment |Â
up vote
0
down vote
We have
$$
|AP|_0 = 15\
|BP|_0 = 5\
r = frac_02\
|AP| = 2rcostheta\
|BP| = 2rsintheta
$$
then
$$
fracAPBP = frac20 cos (theta )-1520 sin (theta )-5 = frac4 cos (theta )-34 sin (theta )-1
$$
the solution follows as in
Calculation of the modulus of elasticity of a stretched string
NOTE
with $lambda$ the elastic modulus,
$$
lambdaleft(fracAPAPright)costheta = lambdaleft(fracBPright)sintheta
$$
(In equilibrium the horizontal projection for $F_AP$ and $F_PB$ are equal) then
$$
fracAPBP=fracsinthetacosthetafracAP
$$
or as expected
$$
frac4 cos theta-34 sintheta-1 = 3left(fracsinthetacosthetaright)
$$
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
add a comment |Â
up vote
0
down vote
up vote
0
down vote
We have
$$
|AP|_0 = 15\
|BP|_0 = 5\
r = frac_02\
|AP| = 2rcostheta\
|BP| = 2rsintheta
$$
then
$$
fracAPBP = frac20 cos (theta )-1520 sin (theta )-5 = frac4 cos (theta )-34 sin (theta )-1
$$
the solution follows as in
Calculation of the modulus of elasticity of a stretched string
NOTE
with $lambda$ the elastic modulus,
$$
lambdaleft(fracAPAPright)costheta = lambdaleft(fracBPright)sintheta
$$
(In equilibrium the horizontal projection for $F_AP$ and $F_PB$ are equal) then
$$
fracAPBP=fracsinthetacosthetafracAP
$$
or as expected
$$
frac4 cos theta-34 sintheta-1 = 3left(fracsinthetacosthetaright)
$$
We have
$$
|AP|_0 = 15\
|BP|_0 = 5\
r = frac_02\
|AP| = 2rcostheta\
|BP| = 2rsintheta
$$
then
$$
fracAPBP = frac20 cos (theta )-1520 sin (theta )-5 = frac4 cos (theta )-34 sin (theta )-1
$$
the solution follows as in
Calculation of the modulus of elasticity of a stretched string
NOTE
with $lambda$ the elastic modulus,
$$
lambdaleft(fracAPAPright)costheta = lambdaleft(fracBPright)sintheta
$$
(In equilibrium the horizontal projection for $F_AP$ and $F_PB$ are equal) then
$$
fracAPBP=fracsinthetacosthetafracAP
$$
or as expected
$$
frac4 cos theta-34 sintheta-1 = 3left(fracsinthetacosthetaright)
$$
edited Jul 16 at 18:25
answered Jul 16 at 16:24
Cesareo
5,7922412
5,7922412
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
add a comment |Â
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
Thanks very much for your work. I'll try an learn from it! Mitch.
– gnitsuk
Jul 18 at 9:21
add a comment |Â
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It could be that your assumption that the new point is exactly below the old point, is not right. The force equilibrium in the horizontal tells that the forces have to be equal on both sides, which leads to that the (absolute) elongation has to be equal on both sides.
– Matti P.
Jul 16 at 11:58