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Exponential Integral Table
51 points
x from -5 step 0.2
First row x = -5, Ei = -0.0011483
Last row x = 5, Ei = 40.18527536
x Ei(x)
-5 -0.0011482956
-4.8 -0.0014529939
-4.6 -0.0018410058
-4.4 -0.00233601
-4.2 -0.0029687622
-4 -0.0037793524
-3.8 -0.0048202468
-3.6 -0.0061604143
-3.4 -0.0078909735
-3.2 -0.0101329925
-3 -0.0130483811
-2.8 -0.0168552924
-2.6 -0.0218502218
-2.4 -0.0284402609
-2.2 -0.0371911371
-2 -0.0489005107
-1.8 -0.0647131294
-1.6 -0.0863083337
-1.4 -0.1162193126
-1.2 -0.1584084369
-1 -0.2193839344
-0.8 -0.3105965785
-0.6 -0.4543795032
-0.4 -0.7023801189
-0.2 -1.2226505442
0 NaN
0.2 -0.8217605879
0.4 0.1047652186
0.6 0.7698812899
0.8 1.3473965482
1 1.8951178164
1.2 2.4420922852
1.4 3.0072074642
1.6 3.605319949
1.8 4.2498675575
2 4.954234356
2.2 5.7326146998
2.4 6.6006702764
2.6 7.5761147698
2.8 8.6792977238
3 9.9338325706
3.2 11.367302657
3.4 13.0120753041
3.6 14.9062540995
3.8 17.0948022652
4 19.6308744701
4.2 22.5774006478
4.4 26.0089732716
4.6 30.0140992965
4.8 34.6978898738
5 40.1852753558

What is the Exponential Integral Ei(x) Table Calculator?

This tool builds a table of the exponential integral Ei(x) over an evenly spaced sequence of x values. You choose a starting value, a step size, and how many points you want, and it computes Ei at each x. The exponential integral is a special function that appears throughout physics and engineering, including radiative transfer, electron-beam simulation, and the asymptotic analysis of integrals.

How to Use It

Enter the initial value of x (the first row), the increment added to x for each successive row, and the number of points (rows). The x value of row n is \(x_n = \text{startX} + n \cdot \text{stepX}\) for \(n = 0, 1, \dots, \text{pointCount}-1\). The calculator returns every (x, Ei(x)) pair plus a quick summary of the first and last rows. A step of zero produces a constant column; \(x = 0\) is undefined because Ei has a logarithmic singularity there.

The Formula Explained

The convergent series used is $$\operatorname{Ei}(x_n) = \gamma + \ln|x_n| + \sum_{k=1}^{\infty} \frac{x_n^{\,k}}{k \cdot k!}$$ where \(\gamma\) is the Euler-Mascheroni constant \(0.5772156649\). The absolute value in \(\ln|x|\) together with the alternating powers of x correctly produce Ei on both the positive and negative branches. For large \(|x|\) (beyond about 40) the series suffers cancellation, so an asymptotic expansion \(\operatorname{Ei}(x) \sim (e^x / x) \sum n!/x^n\) is used instead.

Curve of the exponential integral Ei(x) with a vertical asymptote at x equals zero
The Ei(x) curve: it diverges to negative infinity near \(x = 0\) and rises steeply for positive x.

Worked Example

For \(x = 1\): \(\ln|1| = 0\) and the series sum is about \(1.3179022\), so $$\operatorname{Ei}(1) = 0.5772157 + 0 + 1.3179022 = 1.8951178$$ matching the standard tabulated value. Likewise \(\operatorname{Ei}(2) = 4.9542344\) and \(\operatorname{Ei}(-1) = -0.2193839\).

Table of evenly spaced x values mapped to Ei(x) values with arrows
Each evenly spaced x value produces one Ei(x) entry in the output table.

FAQ

Why is \(x = 0\) undefined? Ei(x) has a logarithmic singularity at the origin (\(\ln|x|\) diverges), so the value is reported as not-a-number.

How accurate is the table? The series reproduces standard Ei values to roughly machine precision for moderate \(|x|\), with an asymptotic fallback keeping large arguments stable.

How is Ei different from E1? They are related by \(\operatorname{Ei}(x) = -E_1(-x)\) for \(x < 0\); this calculator returns the principal-value Ei.

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