Given luminous intensity \$I_v\$ in candelas (1 cd = 1000 mcd) and solid angle
in steradians (full sphere being \$4 \pi\$, half-sphere \$2 \pi\$ steradians), luminous flux \$\Phi_v\$ is \$\Phi_v = I_v \Omega\$.
For an omnidirectional (spherical) uniform bulb, luminous flux is about 0.012566 lm/mcd.
For a bulb emitting light at uniform intensity to half-space, luminous flux is about 0.0062832 lm/mcd.
For LEDs, luminous intensity varies depending on the direction, and luminous flux is actually an integral of the direction-dependent luminous intensity over all solid angles (all possible directions).
Technically, candelas describe the (wavelength-weighted) power emitted by the light source in a particular direction. Solid angle describes how much of all possible directions the light source covers (the surface area of an unit-radius sphere), and luminous flux is the total amount of (wavelength-weighted) power emitted by the light source.
Thus, when listed for a LED, the figure in candelas is either a peak or average intensity, and varies depending on direction; and the flux in lumen is the overall amount of light it emits considering all directions. The ratio of the flux to intensity, \$\Omega = \Phi_v / I_v\$, is a rough single-number description of the solid angle it emits light to, or "spread", if you will.