I could not break this equation. Please help meplease help me fit my equation into my margins!List of equations, including equation contents and captionPlease how can I write this equation in latex?help in writing equationequation reference too close to equationLaTex error please helpHow continue a equation next lineI need help to write this equationequation custom horizontal alignment & numbering each rowCan anyone please help me to solve this? No equation number is appearing for this code
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I could not break this equation. Please help me
please help me fit my equation into my margins!List of equations, including equation contents and captionPlease how can I write this equation in latex?help in writing equationequation reference too close to equationLaTex error please helpHow continue a equation next lineI need help to write this equationequation custom horizontal alignment & numbering each rowCan anyone please help me to solve this? No equation number is appearing for this code
3
f_2=fracsqrtfracs-4 textmpsi^2s-4 textme^2 left(16 textca textcw textEE^2 g
textgpsi s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^8-64
textca textcw textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4
textmpsi^2+sright) cos (theta ) textmZ^8+8 textca textcw textEE^2 g textgpsi s^4
cos (theta ) textmZ^6-32 textca textcw textEE^2 g textgpsi textme^2 s^3 cos
(theta ) textmZ^6+16 textca textcw textEE^2 g textgpsi s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^6-64 textca textcw
textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma
^2 cos (theta ) textmZ^6-40 textca textcw textEE^2 g textgpsi s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^6+160 textca textcw textEE^2 g
textgpsi textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^6-16 textca textcw textEE^2 g textgpsi s^5 cos (theta ) textmZ^4+64
textca textcw textEE^2 g textgpsi textme^2 s^4 cos (theta ) textmZ^4+8 textca
textcw textEE^2 g textgpsi s^4 Gamma ^2 cos (theta ) textmZ^4-32 textca textcw
textEE^2 g textgpsi textme^2 s^3 Gamma ^2 cos (theta ) textmZ^4-8 textca textcw
textEE^2 g textgpsi s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma ^2 cos
(theta ) textmZ^4+32 textca textcw textEE^2 g textgpsi textme^2 s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^4+32 textca textcw
textEE^2 g textgpsi s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^4-128 textca textcw textEE^2 g textgpsi textme^2 s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^4-8 a textca textcv g^2
textgpsi^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+32 a textca textcv g^2 textgpsi^2
textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+8 textca textcw textEE^2 g
textgpsi s^6 cos (theta ) textmZ^2-32 textca textcw textEE^2 g textgpsi textme^2
s^5 cos (theta ) textmZ^2-8 textca textcw textEE^2 g textgpsi s^5 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^2+32 textca textcw textEE^2 g
textgpsi textme^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^2-8 a textca textcv g^2 textgpsi^2 s^5 sqrttextmZ^4+left(Gamma ^2-2 sright)
textmZ^2+s^2 cos (theta ) textmZ^2+32 a textca textcv g^2 textgpsi^2 textme^2 s^4
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2+8 a textca
textcv g^2 textgpsi^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2-32 a textca
textcv g^2 textgpsi^2 textme^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2right) theta
left(s-4 textmpsi^2right)256 textcw^2 textmZ^4 pi ^2 s^3 left(textmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2right)^3/2
equations
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
add a comment |
3
f_2=fracsqrtfracs-4 textmpsi^2s-4 textme^2 left(16 textca textcw textEE^2 g
textgpsi s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^8-64
textca textcw textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4
textmpsi^2+sright) cos (theta ) textmZ^8+8 textca textcw textEE^2 g textgpsi s^4
cos (theta ) textmZ^6-32 textca textcw textEE^2 g textgpsi textme^2 s^3 cos
(theta ) textmZ^6+16 textca textcw textEE^2 g textgpsi s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^6-64 textca textcw
textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma
^2 cos (theta ) textmZ^6-40 textca textcw textEE^2 g textgpsi s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^6+160 textca textcw textEE^2 g
textgpsi textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^6-16 textca textcw textEE^2 g textgpsi s^5 cos (theta ) textmZ^4+64
textca textcw textEE^2 g textgpsi textme^2 s^4 cos (theta ) textmZ^4+8 textca
textcw textEE^2 g textgpsi s^4 Gamma ^2 cos (theta ) textmZ^4-32 textca textcw
textEE^2 g textgpsi textme^2 s^3 Gamma ^2 cos (theta ) textmZ^4-8 textca textcw
textEE^2 g textgpsi s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma ^2 cos
(theta ) textmZ^4+32 textca textcw textEE^2 g textgpsi textme^2 s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^4+32 textca textcw
textEE^2 g textgpsi s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^4-128 textca textcw textEE^2 g textgpsi textme^2 s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^4-8 a textca textcv g^2
textgpsi^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+32 a textca textcv g^2 textgpsi^2
textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+8 textca textcw textEE^2 g
textgpsi s^6 cos (theta ) textmZ^2-32 textca textcw textEE^2 g textgpsi textme^2
s^5 cos (theta ) textmZ^2-8 textca textcw textEE^2 g textgpsi s^5 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^2+32 textca textcw textEE^2 g
textgpsi textme^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^2-8 a textca textcv g^2 textgpsi^2 s^5 sqrttextmZ^4+left(Gamma ^2-2 sright)
textmZ^2+s^2 cos (theta ) textmZ^2+32 a textca textcv g^2 textgpsi^2 textme^2 s^4
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2+8 a textca
textcv g^2 textgpsi^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2-32 a textca
textcv g^2 textgpsi^2 textme^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2right) theta
left(s-4 textmpsi^2right)256 textcw^2 textmZ^4 pi ^2 s^3 left(textmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2right)^3/2
equations
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
6
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
4
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34
add a comment |
3
3
3
f_2=fracsqrtfracs-4 textmpsi^2s-4 textme^2 left(16 textca textcw textEE^2 g
textgpsi s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^8-64
textca textcw textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4
textmpsi^2+sright) cos (theta ) textmZ^8+8 textca textcw textEE^2 g textgpsi s^4
cos (theta ) textmZ^6-32 textca textcw textEE^2 g textgpsi textme^2 s^3 cos
(theta ) textmZ^6+16 textca textcw textEE^2 g textgpsi s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^6-64 textca textcw
textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma
^2 cos (theta ) textmZ^6-40 textca textcw textEE^2 g textgpsi s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^6+160 textca textcw textEE^2 g
textgpsi textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^6-16 textca textcw textEE^2 g textgpsi s^5 cos (theta ) textmZ^4+64
textca textcw textEE^2 g textgpsi textme^2 s^4 cos (theta ) textmZ^4+8 textca
textcw textEE^2 g textgpsi s^4 Gamma ^2 cos (theta ) textmZ^4-32 textca textcw
textEE^2 g textgpsi textme^2 s^3 Gamma ^2 cos (theta ) textmZ^4-8 textca textcw
textEE^2 g textgpsi s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma ^2 cos
(theta ) textmZ^4+32 textca textcw textEE^2 g textgpsi textme^2 s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^4+32 textca textcw
textEE^2 g textgpsi s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^4-128 textca textcw textEE^2 g textgpsi textme^2 s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^4-8 a textca textcv g^2
textgpsi^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+32 a textca textcv g^2 textgpsi^2
textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+8 textca textcw textEE^2 g
textgpsi s^6 cos (theta ) textmZ^2-32 textca textcw textEE^2 g textgpsi textme^2
s^5 cos (theta ) textmZ^2-8 textca textcw textEE^2 g textgpsi s^5 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^2+32 textca textcw textEE^2 g
textgpsi textme^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^2-8 a textca textcv g^2 textgpsi^2 s^5 sqrttextmZ^4+left(Gamma ^2-2 sright)
textmZ^2+s^2 cos (theta ) textmZ^2+32 a textca textcv g^2 textgpsi^2 textme^2 s^4
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2+8 a textca
textcv g^2 textgpsi^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2-32 a textca
textcv g^2 textgpsi^2 textme^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2right) theta
left(s-4 textmpsi^2right)256 textcw^2 textmZ^4 pi ^2 s^3 left(textmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2right)^3/2
equations
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
f_2=fracsqrtfracs-4 textmpsi^2s-4 textme^2 left(16 textca textcw textEE^2 g
textgpsi s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^8-64
textca textcw textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4
textmpsi^2+sright) cos (theta ) textmZ^8+8 textca textcw textEE^2 g textgpsi s^4
cos (theta ) textmZ^6-32 textca textcw textEE^2 g textgpsi textme^2 s^3 cos
(theta ) textmZ^6+16 textca textcw textEE^2 g textgpsi s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^6-64 textca textcw
textEE^2 g textgpsi textme^2 s sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma
^2 cos (theta ) textmZ^6-40 textca textcw textEE^2 g textgpsi s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^6+160 textca textcw textEE^2 g
textgpsi textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^6-16 textca textcw textEE^2 g textgpsi s^5 cos (theta ) textmZ^4+64
textca textcw textEE^2 g textgpsi textme^2 s^4 cos (theta ) textmZ^4+8 textca
textcw textEE^2 g textgpsi s^4 Gamma ^2 cos (theta ) textmZ^4-32 textca textcw
textEE^2 g textgpsi textme^2 s^3 Gamma ^2 cos (theta ) textmZ^4-8 textca textcw
textEE^2 g textgpsi s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) Gamma ^2 cos
(theta ) textmZ^4+32 textca textcw textEE^2 g textgpsi textme^2 s^2 sqrts left(-4
textme^2+4 textmpsi^2+sright) Gamma ^2 cos (theta ) textmZ^4+32 textca textcw
textEE^2 g textgpsi s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^4-128 textca textcw textEE^2 g textgpsi textme^2 s^3 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^4-8 a textca textcv g^2
textgpsi^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+32 a textca textcv g^2 textgpsi^2
textme^2 s^2 sqrts left(-4 textme^2+4 textmpsi^2+sright) sqrttextmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^4+8 textca textcw textEE^2 g
textgpsi s^6 cos (theta ) textmZ^2-32 textca textcw textEE^2 g textgpsi textme^2
s^5 cos (theta ) textmZ^2-8 textca textcw textEE^2 g textgpsi s^5 sqrts left(-4
textme^2+4 textmpsi^2+sright) cos (theta ) textmZ^2+32 textca textcw textEE^2 g
textgpsi textme^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright) cos (theta )
textmZ^2-8 a textca textcv g^2 textgpsi^2 s^5 sqrttextmZ^4+left(Gamma ^2-2 sright)
textmZ^2+s^2 cos (theta ) textmZ^2+32 a textca textcv g^2 textgpsi^2 textme^2 s^4
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2+8 a textca
textcv g^2 textgpsi^2 s^4 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2-32 a textca
textcv g^2 textgpsi^2 textme^2 s^3 sqrts left(-4 textme^2+4 textmpsi^2+sright)
sqrttextmZ^4+left(Gamma ^2-2 sright) textmZ^2+s^2 cos (theta ) textmZ^2right) theta
left(s-4 textmpsi^2right)256 textcw^2 textmZ^4 pi ^2 s^3 left(textmZ^4+left(Gamma
^2-2 sright) textmZ^2+s^2right)^3/2
equations
equations
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
edited Apr 13 at 19:56
Phelype Oleinik
28.5k64894
28.5k64894
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
asked Apr 13 at 19:56
Sahabub JahediSahabub Jahedi
161
161
6
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
4
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34
add a comment |
6
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
4
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34
6
6
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
4
4
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34
add a comment |
2 Answers
2
active
oldest
votes
5
First, the source needs to be broken up inserting line breaks at suitable places so you can get some idea of the total structure of the formula. An editor that will show you matching parentheses and highlight text according to chosen patterns is a great help here.
It turns out that the formula is a fraction in which most of the text is a parenthesised expression in the denumerator. That needs to be taken out, named, and typeset explicitly. I chose to call this expression Ξ.
Also, there are lots of unnecessary left … right pairs. I deleted those. Further, I replaced text by the more appropriate mathrm. I ended up with the following code. It's a complete, compilable latex document. It still has multiple issues that need to be dealt with before you have a readable output. Most importantly, all the multicharacter variable names need some spacing around them. Use , for that.
documentclassarticle
usepackagemathtools,amsfonts
allowdisplaybreaks[1]
begindocument
beginequation
f_2=frac
sqrtfracs-4 mathrmmpsi^2s-4 mathrmme^2
Xi theta (s-4 mathrmmpsi^2)
256 mathrmcw^2 mathrmmZ^4 pi ^2 s^3
(mathrmmZ^4
+(Gamma ^2-2 s) mathrmmZ^2+s^2)^3/2
endequation
where
beginalign*
Xi&=16 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^8
\&
-64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2 +4 mathrmmpsi^2+s) cos (theta ) mathrmmZ^8
+8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
cos (theta ) mathrmmZ^6
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^3 cos
(theta ) mathrmmZ^6
\&
+16 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-64 mathrmca mathrmcw
mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-40 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^6
\&
+160 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^6
\&
-16 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^5 cos (theta ) mathrmmZ^4
\&
+64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^4
cos (theta ) mathrmmZ^4
\&
+8 mathrmca
mathrmcw mathrmEE^2 g mathrmgpsi s^4 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^3 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-128 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2
mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+8 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^6 cos (theta ) mathrmmZ^2
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^5 cos (theta ) mathrmmZ^2
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^5
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^2
\&
+32 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^2
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^5
sqrtmathrmmZ^4+(Gamma ^2-2 s)
mathrmmZ^2+s^2 cos (theta ) mathrmmZ^2
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^4
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
+8 a mathrmca
mathrmcv g^2 mathrmgpsi^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
-32 a mathrmca
mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
endalign*
enddocument
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
add a comment |
5
There are a lot of repeated items in your equation. I suggest you do something like the following, which (a) eliminates all left and right sizing directives (this is necessary because left and right disallow line breaks) and expresses f_2 as the product and ratio of less-complex items. The repeated items are treated as new variables named psi, phi, kappa, and lambda; you're obviously free to come up with more descriptive variable names.
documentclassarticle
usepackagemathtools
newcommandvn[1]mathrm,#1
begindocument
noindent
Put
$psi=sqrtsmash[b]s (-4 vnme^2+4 vnmpsi^2+s)$,
$phi=sqrtsmash[b]vnmZ^4 +(Gamma^2-2 s) vnmZ^2+s^2$,
$kappa= vnca vncw vnEE^2, g vngpsicostheta$, and
$lambda=vnca vncv, g^2 vngpsi^2costheta$.
Then
beginalign*
f_2 &=ucdot vcdot theta(s-4 vnmpsi^2)/w, \
shortintertextwhere
u &= biggl(fracs-4 vnmpsi^2s-4 vnme^2biggr)^!1/2 \
v &=beginaligned[t]
&16 kappa s^2 psi vnmZ^8
-64 kappa vnme^2 s psi vnmZ^8
\&+8 kappa s^4 vnmZ^6
-32 kappa vnme^2 s^3 vnmZ^6
\&+16 kappa s^2 psi Gamma^2 vnmZ^6
-64 kappa vnme^2 s psi Gamma^2 vnmZ^6
\&-40 kappa s^3 psi vnmZ^6
+160kappa vnme^2 s^2 psi vnmZ^6
\&-16 kappa s^5 vnmZ^4
+64 kappa vnme^2 s^4 vnmZ^4
\&+8 kappa s^4 Gamma^2 vnmZ^4
-32 kappa vnme^2 s^3 Gamma^2 vnmZ^4
\&-8 kappa s^3 psi Gamma^2 vnmZ^4
+32 kappa vnme^2 s^2 psi Gamma^2 vnmZ^4
\&+32 kappa s^4 psi vnmZ^4
-128kappa vnme^2 s^3 psi vnmZ^4
\&+8 kappa s^6 vnmZ^2
-32 kappa vnme^2 s^5 vnmZ^2
\&-8 kappa s^5 psi vnmZ^2
+32 kappa vnme^2 s^4 psi vnmZ^2
\&-8 alambda s^3 psi phi vnmZ^4
+32alambda vnme^2 s^2 psi phi vnmZ^4
\&-8 alambda s^5 phi vnmZ^2
+32alambda vnme^2 s^4 psi vnmZ^2
\&+8 alambda s^4 psi phi vnmZ^2
-32alambda vnme^2 s^3 psi phi vnmZ^2
endaligned\
shortintertextand
w &=256 vncw^2 vnmZ^4 pi^2 s^3 phi^3/cos^3theta
endalign*
enddocument
edited Apr 14 at 6:54
Community♦
1
answered Apr 13 at 21:31
MicoMico
292k32402789
add a comment |
Your Answer
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2 Answers
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5
First, the source needs to be broken up inserting line breaks at suitable places so you can get some idea of the total structure of the formula. An editor that will show you matching parentheses and highlight text according to chosen patterns is a great help here.
It turns out that the formula is a fraction in which most of the text is a parenthesised expression in the denumerator. That needs to be taken out, named, and typeset explicitly. I chose to call this expression Ξ.
Also, there are lots of unnecessary left … right pairs. I deleted those. Further, I replaced text by the more appropriate mathrm. I ended up with the following code. It's a complete, compilable latex document. It still has multiple issues that need to be dealt with before you have a readable output. Most importantly, all the multicharacter variable names need some spacing around them. Use , for that.
documentclassarticle
usepackagemathtools,amsfonts
allowdisplaybreaks[1]
begindocument
beginequation
f_2=frac
sqrtfracs-4 mathrmmpsi^2s-4 mathrmme^2
Xi theta (s-4 mathrmmpsi^2)
256 mathrmcw^2 mathrmmZ^4 pi ^2 s^3
(mathrmmZ^4
+(Gamma ^2-2 s) mathrmmZ^2+s^2)^3/2
endequation
where
beginalign*
Xi&=16 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^8
\&
-64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2 +4 mathrmmpsi^2+s) cos (theta ) mathrmmZ^8
+8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
cos (theta ) mathrmmZ^6
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^3 cos
(theta ) mathrmmZ^6
\&
+16 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-64 mathrmca mathrmcw
mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-40 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^6
\&
+160 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^6
\&
-16 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^5 cos (theta ) mathrmmZ^4
\&
+64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^4
cos (theta ) mathrmmZ^4
\&
+8 mathrmca
mathrmcw mathrmEE^2 g mathrmgpsi s^4 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^3 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-128 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2
mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+8 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^6 cos (theta ) mathrmmZ^2
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^5 cos (theta ) mathrmmZ^2
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^5
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^2
\&
+32 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^2
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^5
sqrtmathrmmZ^4+(Gamma ^2-2 s)
mathrmmZ^2+s^2 cos (theta ) mathrmmZ^2
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^4
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
+8 a mathrmca
mathrmcv g^2 mathrmgpsi^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
-32 a mathrmca
mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
endalign*
enddocument
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
add a comment |
5
First, the source needs to be broken up inserting line breaks at suitable places so you can get some idea of the total structure of the formula. An editor that will show you matching parentheses and highlight text according to chosen patterns is a great help here.
It turns out that the formula is a fraction in which most of the text is a parenthesised expression in the denumerator. That needs to be taken out, named, and typeset explicitly. I chose to call this expression Ξ.
Also, there are lots of unnecessary left … right pairs. I deleted those. Further, I replaced text by the more appropriate mathrm. I ended up with the following code. It's a complete, compilable latex document. It still has multiple issues that need to be dealt with before you have a readable output. Most importantly, all the multicharacter variable names need some spacing around them. Use , for that.
documentclassarticle
usepackagemathtools,amsfonts
allowdisplaybreaks[1]
begindocument
beginequation
f_2=frac
sqrtfracs-4 mathrmmpsi^2s-4 mathrmme^2
Xi theta (s-4 mathrmmpsi^2)
256 mathrmcw^2 mathrmmZ^4 pi ^2 s^3
(mathrmmZ^4
+(Gamma ^2-2 s) mathrmmZ^2+s^2)^3/2
endequation
where
beginalign*
Xi&=16 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^8
\&
-64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2 +4 mathrmmpsi^2+s) cos (theta ) mathrmmZ^8
+8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
cos (theta ) mathrmmZ^6
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^3 cos
(theta ) mathrmmZ^6
\&
+16 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-64 mathrmca mathrmcw
mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-40 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^6
\&
+160 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^6
\&
-16 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^5 cos (theta ) mathrmmZ^4
\&
+64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^4
cos (theta ) mathrmmZ^4
\&
+8 mathrmca
mathrmcw mathrmEE^2 g mathrmgpsi s^4 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^3 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-128 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2
mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+8 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^6 cos (theta ) mathrmmZ^2
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^5 cos (theta ) mathrmmZ^2
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^5
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^2
\&
+32 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^2
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^5
sqrtmathrmmZ^4+(Gamma ^2-2 s)
mathrmmZ^2+s^2 cos (theta ) mathrmmZ^2
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^4
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
+8 a mathrmca
mathrmcv g^2 mathrmgpsi^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
-32 a mathrmca
mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
endalign*
enddocument
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
add a comment |
5
5
5
First, the source needs to be broken up inserting line breaks at suitable places so you can get some idea of the total structure of the formula. An editor that will show you matching parentheses and highlight text according to chosen patterns is a great help here.
It turns out that the formula is a fraction in which most of the text is a parenthesised expression in the denumerator. That needs to be taken out, named, and typeset explicitly. I chose to call this expression Ξ.
Also, there are lots of unnecessary left … right pairs. I deleted those. Further, I replaced text by the more appropriate mathrm. I ended up with the following code. It's a complete, compilable latex document. It still has multiple issues that need to be dealt with before you have a readable output. Most importantly, all the multicharacter variable names need some spacing around them. Use , for that.
documentclassarticle
usepackagemathtools,amsfonts
allowdisplaybreaks[1]
begindocument
beginequation
f_2=frac
sqrtfracs-4 mathrmmpsi^2s-4 mathrmme^2
Xi theta (s-4 mathrmmpsi^2)
256 mathrmcw^2 mathrmmZ^4 pi ^2 s^3
(mathrmmZ^4
+(Gamma ^2-2 s) mathrmmZ^2+s^2)^3/2
endequation
where
beginalign*
Xi&=16 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^8
\&
-64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2 +4 mathrmmpsi^2+s) cos (theta ) mathrmmZ^8
+8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
cos (theta ) mathrmmZ^6
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^3 cos
(theta ) mathrmmZ^6
\&
+16 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-64 mathrmca mathrmcw
mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-40 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^6
\&
+160 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^6
\&
-16 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^5 cos (theta ) mathrmmZ^4
\&
+64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^4
cos (theta ) mathrmmZ^4
\&
+8 mathrmca
mathrmcw mathrmEE^2 g mathrmgpsi s^4 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^3 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-128 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2
mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+8 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^6 cos (theta ) mathrmmZ^2
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^5 cos (theta ) mathrmmZ^2
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^5
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^2
\&
+32 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^2
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^5
sqrtmathrmmZ^4+(Gamma ^2-2 s)
mathrmmZ^2+s^2 cos (theta ) mathrmmZ^2
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^4
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
+8 a mathrmca
mathrmcv g^2 mathrmgpsi^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
-32 a mathrmca
mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
endalign*
enddocument
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
First, the source needs to be broken up inserting line breaks at suitable places so you can get some idea of the total structure of the formula. An editor that will show you matching parentheses and highlight text according to chosen patterns is a great help here.
It turns out that the formula is a fraction in which most of the text is a parenthesised expression in the denumerator. That needs to be taken out, named, and typeset explicitly. I chose to call this expression Ξ.
Also, there are lots of unnecessary left … right pairs. I deleted those. Further, I replaced text by the more appropriate mathrm. I ended up with the following code. It's a complete, compilable latex document. It still has multiple issues that need to be dealt with before you have a readable output. Most importantly, all the multicharacter variable names need some spacing around them. Use , for that.
documentclassarticle
usepackagemathtools,amsfonts
allowdisplaybreaks[1]
begindocument
beginequation
f_2=frac
sqrtfracs-4 mathrmmpsi^2s-4 mathrmme^2
Xi theta (s-4 mathrmmpsi^2)
256 mathrmcw^2 mathrmmZ^4 pi ^2 s^3
(mathrmmZ^4
+(Gamma ^2-2 s) mathrmmZ^2+s^2)^3/2
endequation
where
beginalign*
Xi&=16 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^8
\&
-64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2 +4 mathrmmpsi^2+s) cos (theta ) mathrmmZ^8
+8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
cos (theta ) mathrmmZ^6
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^3 cos
(theta ) mathrmmZ^6
\&
+16 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-64 mathrmca mathrmcw
mathrmEE^2 g mathrmgpsi mathrmme^2 s
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^6
\&
-40 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^6
\&
+160 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^6
\&
-16 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi s^5 cos (theta ) mathrmmZ^4
\&
+64 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2 s^4
cos (theta ) mathrmmZ^4
\&
+8 mathrmca
mathrmcw mathrmEE^2 g mathrmgpsi s^4 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^3 Gamma ^2 cos (theta ) mathrmmZ^4
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
Gamma ^2 cos (theta ) mathrmmZ^4
\&
+32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-128 mathrmca mathrmcw mathrmEE^2
g mathrmgpsi mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^4
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2
mathrmme^2 s^2
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^4
\&
+8 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi s^6 cos (theta ) mathrmmZ^2
-32 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi mathrmme^2
s^5 cos (theta ) mathrmmZ^2
\&
-8 mathrmca mathrmcw mathrmEE^2 g mathrmgpsi s^5
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
cos (theta ) mathrmmZ^2
\&
+32 mathrmca mathrmcw mathrmEE^2 g
mathrmgpsi mathrmme^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s) cos (theta )
mathrmmZ^2
\&
-8 a mathrmca mathrmcv g^2 mathrmgpsi^2 s^5
sqrtmathrmmZ^4+(Gamma ^2-2 s)
mathrmmZ^2+s^2 cos (theta ) mathrmmZ^2
\&
+32 a mathrmca mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^4
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
+8 a mathrmca
mathrmcv g^2 mathrmgpsi^2 s^4
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
\&
-32 a mathrmca
mathrmcv g^2 mathrmgpsi^2 mathrmme^2 s^3
sqrts (-4 mathrmme^2+4 mathrmmpsi^2+s)
sqrtmathrmmZ^4+(Gamma ^2-2 s) mathrmmZ^2+s^2
cos (theta ) mathrmmZ^2
endalign*
enddocument
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
answered Apr 13 at 20:43
Harald Hanche-OlsenHarald Hanche-Olsen
13.2k24762
13.2k24762
add a comment |
add a comment |
5
There are a lot of repeated items in your equation. I suggest you do something like the following, which (a) eliminates all left and right sizing directives (this is necessary because left and right disallow line breaks) and expresses f_2 as the product and ratio of less-complex items. The repeated items are treated as new variables named psi, phi, kappa, and lambda; you're obviously free to come up with more descriptive variable names.
documentclassarticle
usepackagemathtools
newcommandvn[1]mathrm,#1
begindocument
noindent
Put
$psi=sqrtsmash[b]s (-4 vnme^2+4 vnmpsi^2+s)$,
$phi=sqrtsmash[b]vnmZ^4 +(Gamma^2-2 s) vnmZ^2+s^2$,
$kappa= vnca vncw vnEE^2, g vngpsicostheta$, and
$lambda=vnca vncv, g^2 vngpsi^2costheta$.
Then
beginalign*
f_2 &=ucdot vcdot theta(s-4 vnmpsi^2)/w, \
shortintertextwhere
u &= biggl(fracs-4 vnmpsi^2s-4 vnme^2biggr)^!1/2 \
v &=beginaligned[t]
&16 kappa s^2 psi vnmZ^8
-64 kappa vnme^2 s psi vnmZ^8
\&+8 kappa s^4 vnmZ^6
-32 kappa vnme^2 s^3 vnmZ^6
\&+16 kappa s^2 psi Gamma^2 vnmZ^6
-64 kappa vnme^2 s psi Gamma^2 vnmZ^6
\&-40 kappa s^3 psi vnmZ^6
+160kappa vnme^2 s^2 psi vnmZ^6
\&-16 kappa s^5 vnmZ^4
+64 kappa vnme^2 s^4 vnmZ^4
\&+8 kappa s^4 Gamma^2 vnmZ^4
-32 kappa vnme^2 s^3 Gamma^2 vnmZ^4
\&-8 kappa s^3 psi Gamma^2 vnmZ^4
+32 kappa vnme^2 s^2 psi Gamma^2 vnmZ^4
\&+32 kappa s^4 psi vnmZ^4
-128kappa vnme^2 s^3 psi vnmZ^4
\&+8 kappa s^6 vnmZ^2
-32 kappa vnme^2 s^5 vnmZ^2
\&-8 kappa s^5 psi vnmZ^2
+32 kappa vnme^2 s^4 psi vnmZ^2
\&-8 alambda s^3 psi phi vnmZ^4
+32alambda vnme^2 s^2 psi phi vnmZ^4
\&-8 alambda s^5 phi vnmZ^2
+32alambda vnme^2 s^4 psi vnmZ^2
\&+8 alambda s^4 psi phi vnmZ^2
-32alambda vnme^2 s^3 psi phi vnmZ^2
endaligned\
shortintertextand
w &=256 vncw^2 vnmZ^4 pi^2 s^3 phi^3/cos^3theta
endalign*
enddocument
edited Apr 14 at 6:54
Community♦
1
answered Apr 13 at 21:31
MicoMico
292k32402789
add a comment |
5
There are a lot of repeated items in your equation. I suggest you do something like the following, which (a) eliminates all left and right sizing directives (this is necessary because left and right disallow line breaks) and expresses f_2 as the product and ratio of less-complex items. The repeated items are treated as new variables named psi, phi, kappa, and lambda; you're obviously free to come up with more descriptive variable names.
documentclassarticle
usepackagemathtools
newcommandvn[1]mathrm,#1
begindocument
noindent
Put
$psi=sqrtsmash[b]s (-4 vnme^2+4 vnmpsi^2+s)$,
$phi=sqrtsmash[b]vnmZ^4 +(Gamma^2-2 s) vnmZ^2+s^2$,
$kappa= vnca vncw vnEE^2, g vngpsicostheta$, and
$lambda=vnca vncv, g^2 vngpsi^2costheta$.
Then
beginalign*
f_2 &=ucdot vcdot theta(s-4 vnmpsi^2)/w, \
shortintertextwhere
u &= biggl(fracs-4 vnmpsi^2s-4 vnme^2biggr)^!1/2 \
v &=beginaligned[t]
&16 kappa s^2 psi vnmZ^8
-64 kappa vnme^2 s psi vnmZ^8
\&+8 kappa s^4 vnmZ^6
-32 kappa vnme^2 s^3 vnmZ^6
\&+16 kappa s^2 psi Gamma^2 vnmZ^6
-64 kappa vnme^2 s psi Gamma^2 vnmZ^6
\&-40 kappa s^3 psi vnmZ^6
+160kappa vnme^2 s^2 psi vnmZ^6
\&-16 kappa s^5 vnmZ^4
+64 kappa vnme^2 s^4 vnmZ^4
\&+8 kappa s^4 Gamma^2 vnmZ^4
-32 kappa vnme^2 s^3 Gamma^2 vnmZ^4
\&-8 kappa s^3 psi Gamma^2 vnmZ^4
+32 kappa vnme^2 s^2 psi Gamma^2 vnmZ^4
\&+32 kappa s^4 psi vnmZ^4
-128kappa vnme^2 s^3 psi vnmZ^4
\&+8 kappa s^6 vnmZ^2
-32 kappa vnme^2 s^5 vnmZ^2
\&-8 kappa s^5 psi vnmZ^2
+32 kappa vnme^2 s^4 psi vnmZ^2
\&-8 alambda s^3 psi phi vnmZ^4
+32alambda vnme^2 s^2 psi phi vnmZ^4
\&-8 alambda s^5 phi vnmZ^2
+32alambda vnme^2 s^4 psi vnmZ^2
\&+8 alambda s^4 psi phi vnmZ^2
-32alambda vnme^2 s^3 psi phi vnmZ^2
endaligned\
shortintertextand
w &=256 vncw^2 vnmZ^4 pi^2 s^3 phi^3/cos^3theta
endalign*
enddocument
edited Apr 14 at 6:54
Community♦
1
answered Apr 13 at 21:31
MicoMico
292k32402789
add a comment |
5
5
5
There are a lot of repeated items in your equation. I suggest you do something like the following, which (a) eliminates all left and right sizing directives (this is necessary because left and right disallow line breaks) and expresses f_2 as the product and ratio of less-complex items. The repeated items are treated as new variables named psi, phi, kappa, and lambda; you're obviously free to come up with more descriptive variable names.
documentclassarticle
usepackagemathtools
newcommandvn[1]mathrm,#1
begindocument
noindent
Put
$psi=sqrtsmash[b]s (-4 vnme^2+4 vnmpsi^2+s)$,
$phi=sqrtsmash[b]vnmZ^4 +(Gamma^2-2 s) vnmZ^2+s^2$,
$kappa= vnca vncw vnEE^2, g vngpsicostheta$, and
$lambda=vnca vncv, g^2 vngpsi^2costheta$.
Then
beginalign*
f_2 &=ucdot vcdot theta(s-4 vnmpsi^2)/w, \
shortintertextwhere
u &= biggl(fracs-4 vnmpsi^2s-4 vnme^2biggr)^!1/2 \
v &=beginaligned[t]
&16 kappa s^2 psi vnmZ^8
-64 kappa vnme^2 s psi vnmZ^8
\&+8 kappa s^4 vnmZ^6
-32 kappa vnme^2 s^3 vnmZ^6
\&+16 kappa s^2 psi Gamma^2 vnmZ^6
-64 kappa vnme^2 s psi Gamma^2 vnmZ^6
\&-40 kappa s^3 psi vnmZ^6
+160kappa vnme^2 s^2 psi vnmZ^6
\&-16 kappa s^5 vnmZ^4
+64 kappa vnme^2 s^4 vnmZ^4
\&+8 kappa s^4 Gamma^2 vnmZ^4
-32 kappa vnme^2 s^3 Gamma^2 vnmZ^4
\&-8 kappa s^3 psi Gamma^2 vnmZ^4
+32 kappa vnme^2 s^2 psi Gamma^2 vnmZ^4
\&+32 kappa s^4 psi vnmZ^4
-128kappa vnme^2 s^3 psi vnmZ^4
\&+8 kappa s^6 vnmZ^2
-32 kappa vnme^2 s^5 vnmZ^2
\&-8 kappa s^5 psi vnmZ^2
+32 kappa vnme^2 s^4 psi vnmZ^2
\&-8 alambda s^3 psi phi vnmZ^4
+32alambda vnme^2 s^2 psi phi vnmZ^4
\&-8 alambda s^5 phi vnmZ^2
+32alambda vnme^2 s^4 psi vnmZ^2
\&+8 alambda s^4 psi phi vnmZ^2
-32alambda vnme^2 s^3 psi phi vnmZ^2
endaligned\
shortintertextand
w &=256 vncw^2 vnmZ^4 pi^2 s^3 phi^3/cos^3theta
endalign*
enddocument
edited Apr 14 at 6:54
Community♦
1
answered Apr 13 at 21:31
MicoMico
292k32402789
There are a lot of repeated items in your equation. I suggest you do something like the following, which (a) eliminates all left and right sizing directives (this is necessary because left and right disallow line breaks) and expresses f_2 as the product and ratio of less-complex items. The repeated items are treated as new variables named psi, phi, kappa, and lambda; you're obviously free to come up with more descriptive variable names.
documentclassarticle
usepackagemathtools
newcommandvn[1]mathrm,#1
begindocument
noindent
Put
$psi=sqrtsmash[b]s (-4 vnme^2+4 vnmpsi^2+s)$,
$phi=sqrtsmash[b]vnmZ^4 +(Gamma^2-2 s) vnmZ^2+s^2$,
$kappa= vnca vncw vnEE^2, g vngpsicostheta$, and
$lambda=vnca vncv, g^2 vngpsi^2costheta$.
Then
beginalign*
f_2 &=ucdot vcdot theta(s-4 vnmpsi^2)/w, \
shortintertextwhere
u &= biggl(fracs-4 vnmpsi^2s-4 vnme^2biggr)^!1/2 \
v &=beginaligned[t]
&16 kappa s^2 psi vnmZ^8
-64 kappa vnme^2 s psi vnmZ^8
\&+8 kappa s^4 vnmZ^6
-32 kappa vnme^2 s^3 vnmZ^6
\&+16 kappa s^2 psi Gamma^2 vnmZ^6
-64 kappa vnme^2 s psi Gamma^2 vnmZ^6
\&-40 kappa s^3 psi vnmZ^6
+160kappa vnme^2 s^2 psi vnmZ^6
\&-16 kappa s^5 vnmZ^4
+64 kappa vnme^2 s^4 vnmZ^4
\&+8 kappa s^4 Gamma^2 vnmZ^4
-32 kappa vnme^2 s^3 Gamma^2 vnmZ^4
\&-8 kappa s^3 psi Gamma^2 vnmZ^4
+32 kappa vnme^2 s^2 psi Gamma^2 vnmZ^4
\&+32 kappa s^4 psi vnmZ^4
-128kappa vnme^2 s^3 psi vnmZ^4
\&+8 kappa s^6 vnmZ^2
-32 kappa vnme^2 s^5 vnmZ^2
\&-8 kappa s^5 psi vnmZ^2
+32 kappa vnme^2 s^4 psi vnmZ^2
\&-8 alambda s^3 psi phi vnmZ^4
+32alambda vnme^2 s^2 psi phi vnmZ^4
\&-8 alambda s^5 phi vnmZ^2
+32alambda vnme^2 s^4 psi vnmZ^2
\&+8 alambda s^4 psi phi vnmZ^2
-32alambda vnme^2 s^3 psi phi vnmZ^2
endaligned\
shortintertextand
w &=256 vncw^2 vnmZ^4 pi^2 s^3 phi^3/cos^3theta
endalign*
enddocument
edited Apr 14 at 6:54
Community♦
1
answered Apr 13 at 21:31
MicoMico
292k32402789
edited Apr 14 at 6:54
Community♦
1
edited Apr 14 at 6:54
Community♦
1
edited Apr 14 at 6:54
Community♦
1
1
answered Apr 13 at 21:31
MicoMico
292k32402789
answered Apr 13 at 21:31
MicoMico
292k32402789
answered Apr 13 at 21:31
MicoMico
292k32402789
292k32402789
add a comment |
add a comment |
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6
Let me guess: This was generated by some computer algebra system, Maple perhaps?
– Harald Hanche-Olsen
Apr 13 at 20:13
4
I don't think breaking the equation into separate lines will help with the readability. It's a mess. Go back to maple and try to find a better output. Or start by finding where the fraction switches, and print the numerator and denominator separately.
– Teepeemm
Apr 13 at 20:34