GATE CH flashcards
GATE CH · Build recall with a focused review session.
32 cards. Read the term and the definition here. The deck at the top of this page is optional.
- Overall material balance
- For a steady-state unit with no reaction, total mass in equals total mass out. With reaction, use component balances with generation terms; C independent component balances exist for C species.
- Recycle ratio
- Ratio of recycled stream flow to fresh feed flow. It changes the reactor inlet concentration and per-pass conversion but not the overall conversion for a fixed separator performance.
- Kirchhoff's law
- Relates heat of reaction at one temperature to another: ΔH_r(T2) = ΔH_r(T1) + ∫(T1 to T2) ΔC_p dT, where ΔC_p is the product-minus-reactant heat capacity difference.
- Adiabatic temperature rise
- Maximum temperature increase in an adiabatic reactor at full conversion: ΔT_ad = (−ΔH_r)·X/(Σ Θ_i C_p,i). It sets the vertical span of the operating line on a T-versus-conversion plot.
- Relative volatility
- α_ij = (y_i/x_i)/(y_j/x_j), equal to P_i^sat/P_j^sat for ideal Raoult's law systems. Values near 1 mean difficult separation; α below 1 means component i is heavier.
- Log-mean temperature difference
- ΔT_lm = (ΔT1 − ΔT2)/ln(ΔT1/ΔT2) for countercurrent or cocurrent exchangers. Use it with Q = UAΔT_lm and a correction factor F for multipass shell-and-tube units.
- CSTR versus PFR volume
- For first-order kinetics at equal conversion and feed rate, V_CSTR = vX/[k(1−X)] and V_PFR = (v/k)ln[1/(1−X)]. The CSTR is always larger because it operates at the low outlet concentration.
- Ergun equation
- Predicts pressure drop through a packed bed as the sum of viscous (150μu(1−ε)²/(ε³d_p²)) and inertial (1.75ρu²(1−ε)/(ε³d_p)) terms per unit bed length.
- Hatta number
- Ha = √(kD_AB)/k_c compares reaction rate to diffusion rate in a film. Large Ha means fast reaction confined near the interface; small Ha means the reaction is slow relative to diffusion.
- Fenske equation
- Gives minimum theoretical stages at total reflux: N_min = ln[(x_D/(1−x_D))((1−x_B)/x_B)]/ln α_avg. It assumes constant relative volatility and is used with the Gilliland correlation.
- Kremser equation
- Relates stage count to absorption factor S = L/(mV) in countercurrent absorption or extraction: (Y_N − Y_0)/(Y_1 − Y_0) = (S^(N+1) − S)/(S^(N+1) − 1).
- Integral rate method
- Tests an assumed order by plotting the integrated rate law. First order gives a straight line for −ln(1−X) versus t; second order gives a straight line for X/(1−X) versus t.
- Multiple steady states
- In a non-isothermal CSTR, the S-shaped heat-generation curve can intersect the linear heat-removal line at three points. The middle intersection is unstable and cannot be maintained in practice.
- Azeotrope condition
- At an azeotropic point the vapor and liquid compositions are equal, so y_i = x_i and relative volatility is unity. Ordinary distillation cannot cross this composition barrier.
- Humidity ratio
- Y = 0.622 p_w/(P − p_w) kg water per kg dry air. It is unchanged by heating or cooling without condensation and fixes the position on a psychrometric chart.
- Heat and mass transfer analogy
- Chilton–Colburn analogy equates Nu/Pr^(1/3) with Sh/Sc^(1/3), letting a heat transfer coefficient predict a mass transfer coefficient when the geometries and flow regimes match.
- Ziegler–Nichols reaction curve
- Open-loop tuning from a first-order-plus-dead-time fit: K_c = 1.2τ/(K_p θ), τ_I = 2θ, τ_D = 0.5θ. It gives aggressive settings with roughly quarter-amplitude damping.
- Ultimate gain tuning
- Increase proportional gain until the loop oscillates continuously; record K_cu and period P_u. PID settings are K_c = K_cu/1.7, τ_I = P_u/2, τ_D = P_u/8.
- Routh–Hurwitz criterion
- Builds a table from the closed-loop characteristic polynomial. The number of sign changes in the first column equals the number of right-half-plane roots, so no sign change means stability.
- Decay ratio
- Ratio of successive peak amplitudes in an underdamped response. A decay ratio of one quarter corresponds to a damping coefficient near 0.216 and is a common tuning target.
- Control valve sizing
- Liquid flow through a valve follows Q = C_v√(ΔP/G). Choked flow and cavitation limit the usable pressure drop and must be checked against the vapor pressure.
- HAZOP guide words
- Standard prompts applied to node parameters: NO, MORE, LESS, AS WELL AS, PART OF, REVERSE and OTHER THAN. Each deviation is examined for causes, consequences and safeguards.
- Limiting oxygen concentration
- The maximum oxygen level in a fuel–air–inert mixture that cannot support ignition. Inerting below the LOC, with a safety margin, prevents explosion in vessels and dryers.
- Six-tenths rule
- Scales equipment cost with capacity: C2 = C1(S2/S1)^0.6. The exponent ranges from about 0.4 to 0.9 depending on equipment type and should be checked for the specific item.
- Lang factor
- Multiplies delivered equipment cost to estimate fixed capital investment. Typical values are about 3.1 for solids processing, 4.7 for mixed, and 5.0 for fluid processing plants.
- Van der Waals equation
- Cubic equation of state (P + a/V_m²)(V_m − b) = RT with a = 27R²T_c²/(64P_c) and b = RT_c/(8P_c). It predicts Z_c = 0.375, overestimating the true value near 0.27.
- Fugacity coefficient
- φ_i = f_i/(y_i P) measures departure from ideal-gas behavior. It equals 1 for an ideal gas and is computed by integrating the equation of state over volume.
- Wilson equation limitation
- The Wilson activity coefficient model cannot predict liquid–liquid phase splitting. NRTL and UNIQUAC include the extra interaction parameter needed to represent partially miscible systems.
- Lumped capacitance validity
- Spatially uniform body temperature is assumed when the Biot number hL/k is below 0.1. Then temperature decays exponentially with time constant ρVC_p/(hA).
- Dittus–Boelter correlation
- Nu = 0.023 Re^0.8 Pr^n for turbulent flow in smooth tubes, with n = 0.4 for heating and 0.3 for cooling. Valid for Re above about 10,000 and moderate property variation.
- View factor reciprocity
- For any two surfaces, A_i F_ij = A_j F_ji. Combined with the summation rule Σ F_ij = 1 for an enclosure, it lets unknown view factors be found from known geometry.
- Van 't Hoff equation
- d(ln K)/dT = ΔH°/(RT²). An endothermic reaction has K increasing with temperature; an exothermic one has K decreasing. Integrating assumes constant ΔH° over the range.