[1] Channelled ascent mechanisms include the formation of dykes[3] and ductile fractures that transport the melt in conduits.
When the mantle materials rise, the pressure greatly decreases which significantly lowers the melting point of the rock.
Depending on the efficiency of the segregation and extraction, there will be different structures of the volcanic and igneous plumbing systems.
[1] For instance, if the magma channels are not well connected, the source may not be drained successfully, and dykes may freeze before propagating far enough to feed plutons.
A diapir forms when a blob of buoyant, hot, and ductile magma ascends to a higher lithospheric layer.
[12][5] As the melt is less dense than the surrounding rock, Rayleigh-Taylor instabilities will grow and amplify, and eventually become diapirs.
[12][5] Stoke diapirism is a viable mechanism preferably for the ascent of massive magma bodies in a weak and ductile crust.
[13] Recent studies demonstrated that a dyke-diapir hybrid model may be a more realistic mechanism of diapir formation.
[14] It also demonstrates that episodic injection of magma is crucial in maintaining the temperature of the diapir system and preventing it from freezing.
Therefore, some dykes may rise to the surface, but the majority of them terminates at depth because of solidification of a blockage of rigid layer.
[17] The geometry of the dyke is related to the stress field and the distribution of pre-existing faults and joints in the country rock.
Fault and shear zones act as lines of weakness for magma to flow in and transport to upper levels.
[19] Particularly, a transpressional fault that cuts through layers is related to the transportation and ascent of magma by creating space for emplacement.
[2] From field evidence, the formation of plutons involves multiple stages of magma injection instead of a single pulse.
[21] According to the depth of formation and geometry, magma emplacement can be classified into plutons, sills, laccoliths and lopoliths.
[4] From field evidence, when plutons are formed in a ductile environment, it will displace the surrounding rocks both laterally and vertically.
They may have roots that tapers downwards which eventually become cylindrical-shaped feeder structures which cause the floors to dip inward at different angles.
[1] Sills are generally defined as sheet intrusions which are tabular in shape and dominantly concordant to the surrounding rock layers.
[25] However, in some cases, sills may deform sedimentary layers and exhibit other geometries such as inclined or sub-vertical shapes.
Depending to its shape and concordance to the country rock, sills can be classified into five different types based on field evidence.
[27] Transgressive sills cut through and propagate to higher layers with an oblique angle to the host rock, displaying discordant properties.
[28] They typically display dome-shaped structures with slightly elevated roofs and flat floors that are concordant to rock layers.
[28] These lines of weakness provide pathways for the formation of initial sill-like structures that are horizontal in shape.
[29] After some time, when the cooling rate decreases, and when the sills continue to stack onto one another, sheet intrusion is no longer a favourable mechanism because the zones of weakness diminish.
The cantilever model describes the formation of the lopoliths as a result of the tilting of floor about a point at the pluton margin.