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Spec mapping: AQA 7037, Paper 1 (Physical), §3.1.1 — although the Water and Carbon core foregrounds the basin hydrological cycle, the fluvial processes and landforms developed here support the systems-and-equilibrium framework that runs through the whole unit, and they are directly examinable where the specification asks about the operation of the drainage basin and channel system over time. (They also strongly underpin §3.1.3 Coastal systems and §3.1.5 Hazards through shared process and equilibrium concepts.) This depth lesson goes well beyond an introductory treatment, using the Hjulström curve, competence/capacity, hydraulic geometry and the graded profile to reason quantitatively about channel form. AOs exercised: AO1 (erosion/transport/deposition processes; landform formation), AO2 (applying energy and equilibrium concepts to explain landform assemblages), AO3 (reading the Hjulström curve, calculating hydraulic radius and downstream change).
A river channel is a dynamic geomorphological system in which the available energy (a function of discharge and slope) is expended against friction and the sediment load. Landforms are the expression of how that energy is partitioned between erosion, transport and deposition — and explaining them in those terms, with numbers, is what lifts a response into the top band.
The power available to a river — its stream power — can be expressed as:
Ω=ρgQS
where ρ is water density (~1000 kg/m³), g is gravitational acceleration (9.81 m/s²), Q is discharge (m³/s) and S is channel slope. Stream power rises with both discharge and gradient, so although gradient falls downstream, the large increase in Q means total stream power generally increases towards the mouth. How that power is used — eroding the bed and banks, transporting load, or being dissipated as heat against friction — depends on the sediment supply and the channel's efficiency. This single relationship organises everything that follows.
The Hjulström curve (Filip Hjulström, 1935) relates mean flow velocity to sediment particle size, defining the thresholds of erosion, transport and deposition.
The gap between them is the transport zone: a particle already in motion stays in motion at velocities below those needed to entrain it.
| Particle size | Behaviour on the Hjulström curve |
|---|---|
| Clay/silt (< 0.06 mm) | Disproportionately high entrainment velocity because electrostatic cohesion binds fine particles; once suspended they stay up to near-zero velocities (so clay is deposited only in still water — estuaries, oxbows). |
| Sand (~0.06–2 mm) | The curve reaches its minimum near 0.2–0.5 mm: medium sand is the most easily entrained particle, needing only ~0.2 m/s. |
| Gravel/cobbles (> 2 mm) | Entrainment velocity rises steeply with size because of particle mass; transport and entrainment velocities nearly coincide. |
| Boulders (> 256 mm) | Move only in extreme floods (velocities of metres per second). |
Exam significance: The curve explains why sandy beds are common (sand is mobilised at the lowest velocities), why clay banks resist erosion yet, once eroded, build mudflats and estuarine deposits, and why a falling flood deposits its coarsest load first and its finest last (graded bedding). The single most-missed AO3 reading is the high entrainment velocity for clay — students wrongly assume "small = easy to erode".
Two distinct measures of transport ability:
competence∝V6,capacity∝Q (and V).
Key distinction: A large lowland river in spate has high capacity (vast suspended load) but may have only moderate competence (fine bed), whereas a small steep mountain torrent in flood has high competence (moves cobbles) but low capacity. The V6 law is the most examinable single fact here, because it quantifies the geomorphic dominance of rare high-magnitude floods.
Channel efficiency is measured by the hydraulic radius:
R=PA
where A is the cross-sectional area of flow (m²) and P is the wetted perimeter (m). A larger R means a smaller proportion of the flow is in frictional contact with the bed and banks, so less energy is lost and velocity is higher for a given slope (consistent with Manning's equation from the previous lesson). A semicircle is the theoretically most efficient shape; natural channels approximate a wide, shallow parabola.
Worked illustration. A near-rectangular channel 10 m wide and 2 m deep has A=20 m² and P=10+2+2=14 m, so R=20/14=1.43 m. A narrow, deep channel of the same area — 5 m wide, 4 m deep — has P=5+4+4=13 m and R=20/13=1.54 m, i.e. more efficient despite identical area, because relatively less perimeter is wetted. This is the geometric reason deep channels run faster than shallow ones of equal area.
| Variable | Downstream trend | Reason |
|---|---|---|
| Discharge | Increases | Tributary and groundwater inputs |
| Width | Increases | Bank erosion accommodates more water |
| Depth | Increases | Bed erosion deepens the channel |
| Hydraulic radius | Increases | Depth rises faster than wetted perimeter |
| Velocity | Generally increases | Rising R more than offsets falling gradient |
| Bed sediment size | Decreases | Attrition and selective transport |
| Channel roughness | Decreases | Finer bed, fewer obstructions |
Common misconception: That velocity falls downstream "because the gradient is gentler". Measured mean velocity usually rises downstream because the gain in hydraulic radius (efficiency) outweighs the loss of slope — a counter-intuitive but well-evidenced result first quantified by Leopold and Maddock (1953).
The Reynolds number classifies flow:
Re=μVdρ
where V is velocity, d depth, ρ density and μ dynamic viscosity (Pa·s).
Turbulence matters because the upward components of turbulent eddies provide the lift and drag that entrain sediment; without turbulence a river would have almost no erosive or transporting power. The Reynolds number thus underpins the Hjulström thresholds physically.
The long profile plots channel altitude from source to mouth and is typically a smooth concave curve — steep in the upper course (high potential energy, small discharge), gentler downstream (lower slope, large discharge, high kinetic energy for lateral work).
A graded river (Mackin, 1948) is one whose slope is delicately adjusted so that, over a period of years, the available discharge and channel characteristics provide just the velocity needed to transport the supplied sediment load — a state of dynamic equilibrium. The graded profile is an ideal: real rivers approach but never perfectly attain it, because geology, sediment supply, base level and human activity keep perturbing it. When perturbed, the river adjusts (eroding to lower a steepened reach, depositing to build up a starved one) in a negative-feedback restoration of grade — a direct application of the equilibrium concept that unifies this entire unit.
flowchart LR
PERT[Perturbation
e.g. base-level fall] --> STEEP[Reach steepens]
STEEP --> ERODE[Increased erosion
+ knickpoint retreat]
ERODE --> ADJUST[Slope reduced
towards grade]
ADJUST --> EQ[Dynamic equilibrium
restored]
EQ -. new perturbation .-> PERT
A knickpoint is a sharp break in the long profile, usually a waterfall or rapids. Causes include:
Rejuvenation gives renewed vertical erosive energy, letting a river incise into its own floodplain. Diagnostic landforms include:
| Feature | Location | Process | Form |
|---|---|---|---|
| Point bar | Inner (convex) bank | Deposition by slow inner flow | Gently sloping, sorted sand/gravel |
| Cut bank / river cliff | Outer (concave) bank | Lateral erosion, undercutting | Steep, actively eroding |
Through repeated outer-bank erosion and inner-bank deposition, meanders migrate laterally and downstream, sweeping the channel across the valley floor and laying down a belt of alluvium — the floodplain, further built up by overbank deposition of fine silt during floods (which also raises natural levées along the banks). When a meander neck narrows and is breached in a flood, the loop is cut off and sealed by deposition to form an oxbow lake — a textbook landform recording former lateral migration.
flowchart TB
A[Sinuous meander
neck narrowing] --> B[Flood breaches
the neck]
B --> C[Flow takes
shorter path]
C --> D[Old loop sealed
by deposition]
D --> E[Oxbow lake
later infills to meander scar]
A field group measures velocity and bed-material size at three sites:
| Site | Mean velocity (m/s) | Median bed grain size D50 (mm) |
|---|---|---|
| Upper | 0.45 | 64 (cobbles) |
| Middle | 0.80 | 8 (gravel) |
| Lower | 1.10 | 0.4 (medium sand) |
Describe. Velocity rises downstream (0.45 → 1.10 m/s) while median grain size falls sharply (64 → 0.4 mm).
Manipulate / interpret with Hjulström. At the upper site, 0.45 m/s is below the entrainment velocity for 64 mm cobbles, so these are largely immobile in normal flow (they were emplaced by past floods). At the lower site, 1.10 m/s is far above the ~0.2 m/s needed to entrain 0.4 mm sand, so the bed is actively transported. Percentage change in velocity:
0.451.10−0.45×100=144%.
Explain. Velocity rises because hydraulic radius and discharge increase downstream, outweighing the gentler gradient; grain size falls through attrition (particles round and shrink) and selective transport (finer material is carried furthest). The two trends are linked: the more efficient, higher-velocity lower channel can still only build a sandy bed because the coarse fraction has been comminuted and left upstream.
Evaluate. D50 at a single survey reflects the day's flow, not the formative flood; one set of point measurements cannot capture the V6 competence spikes that actually emplace the coarse upper-course material. The data illustrate the average trend but understate the role of rare events.
The Tees (~137 km, Cross Fell to the North Sea at Teesmouth) displays the full process–landform sequence:
A depth treatment must name the specific processes, not merely list "erosion, transport, deposition".
Erosional processes:
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