About
The de Broglie wavelength
$lambda = h/p = h/(mv)$ ,where:
$h = 6.626 xx 10^(-34) "J"cdot"s"$ is .$p = mv$ is the linear momentum in$"kg"cdot"m/s"$ , for mass$m$ and velocity$v$ .
Given the energy of an X-ray photon as
$E_"photon" = "100 keV" = hnu = (hc)/lambda$ where
$nu$ is the frequency of the photon in$"s"^(-1)$ and$c = 2.998 xx 10^(8) "m/s"$ is the speed of light.
And so, we suppose that the photon wavelength is numerically the same as the electron wavelength. I suppose this could occur if one tried to ionize a core electron for X-ray diffraction.
$lambda = (hc)/E_"photon" = h/(p)$
This gives a wavelength of:
$lambda = (6.626 xx 10^(-34) cancel"J"cdotcancel"s" cdot 2.998 xx 10^(8) "m/"cancel"s")/("100 "cancel"k"cancel"eV" xx (1.602 xx 10^(-19) cancel"J")/(cancel"1 eV") xx (1000 cancel"J")/cancel"1 kJ")$
$= 1.240 xx 10^(-11) "m"$
Knowing the wavelength, we consider the kinetic energy expressed as a function of linear momentum:
$K = 1/2 mv^2 = p^2/(2m)$
Thus, with
$color(blue)(K) = (h//lambda)^2/(2m)$
$= ((6.626 xx 10^(-34) "kg"cdot"m"^(cancel(2))"/s")/(1.240 xx 10^(-11) cancel"m"))^2/(2 cdot 9.109 xx 10^(-31) cancel"kg")$
$=$ $color(blue)ul(1.567 xx 10^(-15) "J")$
Or perhaps in more useful units...
$1.567 xx 10^(-15) cancel"J" xx (cancel"1 eV")/(1.602 xx 10^(-19) cancel"J") xx ("1 keV")/(1000 cancel"eV")$
$=$ $color(blue)ul("9.782 keV")$
So the X-ray electron has a kinetic energy less than