The helium mass fraction is . For the two compositions, and . The mean molecular weight is therefore
At fixed mass and with the same prescribed opacity coefficient, part (a) gives and . Eliminating radius gives
This is the composition shift of a convective pre-main-sequence track. The higher-helium mass fraction case is hotter at a given luminosity, lying to the left of the case in a Hertzsprung-Russell diagram. Its fixed-luminosity temperature ratio is .
Both stars contract, so both and decrease in this particular opacity model. Their nearly vertical Hayashi tracks therefore run downward and slightly to the right, with arrows in that direction:
Figure 1.
Composition-dependent pre-main-sequence tracks with contraction arrows
. Details.
The plotted luminosity and effective temperature are normalized to arbitrary common references; no opacity normalization or absolute age was specified. The comparison holds the given opacity coefficient fixed.
These paths cease to apply when their assumptions fail. Deuterium-burning energy-generation rate can temporarily slow contraction; sustained hydrogen burning ends the purely gravitational phase. Formation of a radiative core breaks the fully convective adiabat and can lead to a Henyey track toward hotter effective temperature. Partial ionization, a changing atmospheric opacity, and electron degeneracy pressure alter the equation of state or boundary relation. Accretion luminosity, changing mass, and magnetic inhibition of convection can also modify a young star's path.
The specific deuterium-burning energy-generation rate is . By stellar homology,
so
Since ,
Use and from part ii. Then
The two track relations also give
Consequently
Equality occurs at
The preceding formulae imply for , not . Thus the inequality printed in the question is reversed relative to its requested intermediate scaling; the exponent is consistent.