| name | turbomachinery |
| description | Turbomachinery — Euler turbine equation, velocity triangles, centrifugal compressors, axial turbines/compressors, specific speed, cavitation, pump selection, turbine efficiency. |
| metadata | {"priority":7,"promptSignals":{"phrases":["turbomachinery","turbine","compressor","centrifugal pump","axial flow","impeller","specific speed","cavitation","NPSH","velocity triangle"],"minScore":3}} |
Turbomachinery — Complete Skill
Euler Turbomachinery Equation
Fundamental Energy Transfer
W_s = U₂V_u2 - U₁V_u1 [J/kg]
W_s = shaft work per unit mass (+ for pump/compressor, - for turbine)
U = blade tip speed = r×ω [m/s]
V_u = absolute tangential (whirl) velocity component [m/s]
Power:
P = ṁ × (U₂V_u2 - U₁V_u1)
Head (pump):
H = (U₂V_u2 - U₁V_u1) / g [m]
Velocity Triangles
Triangle Notation
At any radius: V = absolute velocity, U = blade speed, W = relative velocity
Vector: V = U + W
Components:
V_a = axial velocity (flow velocity)
V_u = tangential (whirl) component
V_r = radial component
Inlet (1) and Exit (2):
α = angle between V and axial direction
β = angle between W and axial direction (blade angle)
tan(α) = V_u / V_a
tan(β) = (V_u - U) / V_a = W_u / V_a
Centrifugal Pump/Compressor Velocity Triangles
Radial machine: V_a1 = V_a2 (approximately)
Zero inlet whirl (V_u1 = 0): W_s = U₂V_u2
V_u2 = U₂ - V_a2/tan(β₂)
Theoretical head (zero inlet whirl):
H_th = U₂²/g - U₂V_a2/(g×tan(β₂))
Slip factor σ = V_u2,actual / V_u2,ideal
σ ≈ 1 - π/z (Stanitz, z = number of blades, backward-swept)
Typical: σ = 0.85-0.95
Centrifugal Pump/Compressor
Performance
Flow rate: Q = V_a × (2πr₂b₂) [m³/s]
b₂ = impeller width at exit [m]
Tip speed: U₂ = π D₂ N/60
Pressure rise:
ΔP = ρ × η_h × U₂ × V_u2 [Pa]
Efficiency:
η_hydraulic = H_actual / H_theoretical (losses: friction, recirculation)
η_mechanical = shaft power in - bearing losses
η_volumetric = useful Q / total Q through impeller
η_total = η_h × η_m × η_v
Centrifugal Compressor (Compressible Flow)
Total pressure ratio: π_c = P₀₂/P₀₁ = [1 + η_c × U₂²/(c_p×T₀₁)]^(γ/(γ-1))
c_p = 1005 J/kgK (air), γ = 1.4 (air)
Pressure coefficient:
ψ = ΔP_total / (½ρU₂²) = 2η_h σ (typical 0.4-0.7)
Flow coefficient:
φ = V_a2 / U₂ (typical 0.2-0.5)
Axial Flow Machines
Stage Work (Axial Compressor/Turbine)
W_s = U(V_u2 - V_u1) = U × ΔV_u
Axial compressor stage:
Degree of reaction: R = 1 - (V_u1 + V_u2)/(2U) = (β₂ - β₁)/(α₂ - α₁ + β₂ - β₁)
50% reaction: symmetric velocity triangles, β₁ = α₂, β₂ = α₁
Axial turbine:
Stage loading: Ψ = W_s/U² = ΔV_u/U
Flow coefficient: Φ = V_a/U
R = 1 - Ψ/2 (50% reaction nozzle and rotor symmetric)
De Haller Criterion (Compressor)
W₂/W₁ ≥ 0.72 (relative velocity deceleration limit, otherwise stall)
Maximum pressure rise per stage limited by diffusion
Dimensionless Parameters & Specific Speed
Specific Speed (Pump)
N_s = N × Q^(1/2) / H^(3/4) [rpm, m³/s, m — SI form]
N_s,US = N × GPM^(1/2) / H_ft^(3/4) [US customary]
N_s (SI) ranges:
N_s < 20: radial/centrifugal (high head, low flow)
20 < N_s < 80: mixed flow
N_s > 80: axial flow (low head, high flow)
Specific Speed (Turbine)
N_sp = N × P^(1/2) / H^(5/4) [rpm, kW, m]
Turbine selection by N_sp:
Pelton wheel: N_sp < 30 (very high head, low flow)
Francis turbine: 30-300 (medium head)
Kaplan turbine: 300-900 (low head, high flow)
Similarity Laws (Affinity Laws)
At constant speed (varying diameter D):
Q ∝ D³, H ∝ D², P ∝ D⁵
At constant diameter (varying speed N):
Q ∝ N, H ∝ N², P ∝ N³
Pump curves: H-Q, η-Q, P-Q — use to find operating point with system curve
Cavitation
NPSH (Net Positive Suction Head)
NPSH_A = (P_s - P_v) / (ρg) + V_s²/(2g) [m]
P_s = absolute suction pressure [Pa]
P_v = vapor pressure at fluid temperature [Pa]
System NPSH_A:
NPSH_A = P_atm/(ρg) ± z_s - h_L - P_v/(ρg)
z_s = suction head (+ if pump above liquid, - if below)
h_L = suction line friction losses [m]
Rule: NPSH_A > NPSH_R + safety margin (1-3 m)
NPSH_R = required by pump (from pump curve)
Thoma cavitation number:
σ = NPSH / H ≥ σ_critical (from pump specific speed)
σ_critical ≈ N_s^(4/3) / 6.33 × 10⁻⁵ (US specific speed)
Cavitation Prevention
- Lower pump elevation (increase z_s negative value)
- Increase suction pipe diameter (reduce h_L)
- Cool fluid (reduce P_v)
- Select pump with lower NPSH_R
- Use inducer (pre-swirl to lower NPSH_R)
Gas Turbine Cycle
Brayton Cycle (Ideal)
η_Brayton = 1 - 1/r_p^((γ-1)/γ)
r_p = P₂/P₁ = pressure ratio
Specific work:
w_net = c_p(T₃ - T₄) - c_p(T₂ - T₁)
T₂/T₁ = r_p^((γ-1)/γ) (ideal compression)
T₄/T₃ = (1/r_p)^((γ-1)/γ) (ideal expansion)
With real efficiencies:
w_compressor = c_p(T₂ - T₁) / η_c
w_turbine = c_p(T₃ - T₄) × η_t
Optimum pressure ratio for max specific work:
r_p,opt = (T₃/T₁)^(γ/(2(γ-1)))
Steam Turbine
Impulse vs. Reaction
Impulse (0% reaction): all pressure drop in nozzle; blade speed ratio u/C₁ ≈ 0.5
Reaction (50%): pressure drops in both nozzle and blade
Stage efficiency (impulse):
η_blade = 2φ²(cos α₁ - φ)(1 + ψcos(β₁-β₂)/cos α₁)
φ = blade speed ratio = U/C₁
Curtis stage (velocity compounded):
2 rows of moving blades with guide vanes; u/C₁ ≈ 0.25; handles high ΔP per stage
Pump Selection Guide
| N_s (SI) | Type | η_max | Application |
|---|
| < 15 | Radial centrifugal | 70-80% | High pressure, low flow |
| 15-40 | Standard centrifugal | 75-88% | General service |
| 40-100 | Mixed flow | 80-88% | Medium head |
| > 100 | Axial flow | 82-88% | Low head, high flow |
Output
Provide: velocity triangle diagram (α, β, U, V, W at inlet/exit), W_s [J/kg], H [m] or ΔP [bar], N_s, NPSH_A vs. NPSH_R comparison, efficiency η_total [%], operating point on H-Q curve, cavitation risk assessment.