image
imagewidth (px)
4
512
latex
stringlengths
1
188
sample_id
stringlengths
16
16
split_tag
stringclasses
1 value
data_type
stringclasses
1 value
e=\sum_{n=0}^{\infty}\frac{1}{n!}
e8400c9434297b1f
train
human
v=\frac{V_{max}S}{K_{m}+S}
8630312b59b909e7
train
human
\Delta v/c=2\times10^{-7}
717127cfcf4a66b9
train
human
b_{i}=\frac{n_{i}}{m_{solv}}
4d6171bdcb7b23fe
train
human
-\frac{x}{||x||^{2}}\in R^{n}
6cd35307a74c578b
train
human
1^{433}\cdot111+\sqrt{5}^{381}
11638324d88c007a
train
human
Bexp(-t)
9e6f094d87713e8a
train
human
\tilde{n}_{i}
6136fc30a84d3e2c
train
human
(\begin{matrix}n+k-1\\ k\end{matrix})
0ad876500365dd16
train
human
(\begin{matrix}n\\ 0\end{matrix})
6e21b9037daaba80
train
human
(\frac{6}{94})^{6^{146}}
301d507db692ba9a
train
human
\frac{dQ}{dt}
ff3cca3c081e19df
train
human
\frac{\partial\phi_{B}}{\partial t}=0
3e8b460d634e4ec1
train
human
\frac{dr}{dt}
2084db762755dd71
train
human
\overline{x}=\frac{\sum fx}{\sum f}
ed8dfc71a4751353
train
human
\frac{\frac{\frac{7}{7}}{1}}{6-440+\sqrt{9}}
b28ca44b770e1fa2
train
human
\phi(h)=\frac{e^{\cdot\frac{h^{2}}{2}}}{\sqrt{2\Pi}}
e119381d1cd6391c
train
human
S
e63bdf0011dbb3eb
train
human
\frac{n(n+1)(2n+1)}{2}
ea5b0d72fcf2734e
train
human
\tilde{C}_{n}
c416f0732e3fe724
train
human
\frac{\partial\Pi}{\partial x_{j}}
c05ad46a152ce993
train
human
f_{c}=\frac{1}{2\pi\tau}=\frac{1}{2\pi RC}
5713c82e2930d2ab
train
human
(\begin{matrix}n\\ n/2\end{matrix})
193d1fc0a393c432
train
human
\sqrt{n}
801633e180f451d0
train
human
S=\int Ldt
1de8d1974d0128ac
train
human
\int\frac{dx}{lnx}
bdc7418cc12e1431
train
human
L\cdot\frac{10.67}{C^{1.85}d^{4.87}}
497c01d70e96cbbc
train
human
x=[\begin{matrix}7.111\\ -3.222\end{matrix}]
148e048cb76b28b6
train
human
W=\int Fdr
4f8903cd2e24a1c0
train
human
\int fg=f(x)\int g
5466e06110fbf0df
train
human
\frac{d^{4}y}{dx^{4}}
8f5cf3b103267669
train
human
(\begin{matrix}1&2\\ 2&1\end{matrix})
4b021deff1166672
train
human
\frac{470^{10}}{7+9^{5}}
9a989608621a87d7
train
human
\frac{\partial^{2}U}{\partial t^{2}}-c^{2}\frac{\partial^{2}U}{\partial x^{2}}=0
159bc1e5c41ba19b
train
human
0\notin\{1,2,3,4,5\}
a3046ef9b45fea69
train
human
\frac{\partial u}{\partial t}-v\beta y=\frac{\tau_{x}}{\rho h}
3dccd26e1d2a60d2
train
human
r,r^{\prime}\in R_{n}
f134d860d038c938
train
human
\sqrt{\Pi}
364ff267df49235d
train
human
e[n]=x[n]-\hat{x}[n]
a067238b63f6baa5
train
human
\underline{P}\equiv(P^{+},\vec{P}_{\perp})
fbe48871b34c3e7b
train
human
\tilde{G}(s)
7df76337fdce2e24
train
human
\hat{z}(t)
836cc98cbd381f51
train
human
exp_{a}^{p}(b)=a^{a^{\cdot^{\cdot^{a^{b}}}}}
70227171c0c35140
train
human
\frac{\partial V_{2}/\partial Y_{2}}{\partial V_{2}/\partial C_{2}}+1=0
2766219b1fbcdf61
train
human
H(\underline{w})
c9ba862fc52bd09d
train
human
\sigma_{j}>0
1db034f10408d362
train
human
M\underline{A}
d591da47813bcac4
train
human
\pi/R
259969627f874a41
train
human
\frac{10^{145}}{\frac{\frac{10}{376}}{234}}
e75efdcb9ac7d1d0
train
human
v=\sqrt{\frac{ke^{2}}{mr}}
9a9bffb9d4ed2998
train
human
p=3\sqrt[3]{uv}
959f9d7c2fafabdf
train
human
\frac{\partial v_{i}}{\partial x_{i}}=0
60bf18e8eda83338
train
human
H_{1}=H\otimes l^{2}(\Gamma)
484f00cbaaf6edc6
train
human
(\frac{\frac{6}{2}}{2})^{8^{453}}
7d4f8296a30295c6
train
human
I=\int e^{x}cos(x)dx
a6b8ce17fe2b913a
train
human
\tilde{O}(m)
a70135cf252ab274
train
human
\sqrt{C}
36421cdf786a7ffb
train
human
||x-y||<\epsilon
248ec62f63c456f2
train
human
\frac{1}{1-X}
c93bba33cf551b1a
train
human
\frac{1/\lambda}{R_{H}}-\frac{1}{n_{1}^{2}}=-\frac{1}{n_{2}^{2}}
c3167d74d96092a9
train
human
(\begin{matrix}-1&-\nu\\ 0&-1\end{matrix})
244d3e61be1d325e
train
human
\dot{V}_{A}/\dot{Q}_{c}
489302bff8c249d5
train
human
\frac{\eta}{l}=Re_{l}^{-3/4}
da3d4995804aeeec
train
human
a_{(\nu_{7})}
488c89d6121413ab
train
human