Solid Brass Test Specimen with Centerline Thermocouple
25 mm diameter, 50 mm length cylinder with miniature calibrated thermocouple at geometric center.
Study the transient quenching of solid metallic cylinders in an agitated water bath, verify the lumped thermal capacitance model (Biot number Bi < 0.1), and determine the convective cooling time constant τ and heat transfer coefficient h. Explore interactive transport phenomena, unit operations simulation, and chemical engineering telemetry.
Ready to sample with Time t = 30.0 s.
Adjust Time t, then execute chemical process trial.
Chemical and process engineering telemetry is evaluated rigorously using 64-bit IEEE 754 precision. Residuals reflect ordinary least-squares regression across successive observations. Continuous data structures support high-fidelity transport phenomena and unit operations modeling.
The transport and thermodynamic models apply within the specified calibrated operating window (10.0 to 60.0 s). Evaluated using a solid brass cylinder (diameter D = 25.0 mm, length L = 50.0 mm, density ρ = 8530 kg/m^3, specific heat c_p = 380 J/(kg·K), thermal conductivity k = 115 W/(m·K), Bi = 0.025). Linear regression models ln(θ/θ_0) versus t to extract k_rate = 0.0320 s^-1.
25 mm diameter, 50 mm length cylinder with miniature calibrated thermocouple at geometric center.
Preheats specimen to uniform initial temperature T_0 = 85.0 ± 0.1 °C.
Maintains quench water at T_inf = 20.0 ± 0.1 °C with continuous high-shear propeller agitation.
Transfers specimen from heater to quench bath in < 0.2 seconds to establish step cooling datum.
Samples centerline and surface temperatures at 10 Hz with 0.02 °C resolution.
Measures specimen mass m = 209.3 g and dimensions to determine volume V and surface area A_s.
Study the transient quenching of solid metallic cylinders in an agitated water bath, verify the lumped thermal capacitance model (Biot number Bi < 0.1), and determine the convective cooling time constant τ and heat transfer coefficient h. Standardized parameter settings: 10.0, 20.0, 30.0, 40.0, 50.0, 60.0 s.
Place the brass cylinder into the heating chamber at 85.0 °C; monitor centerline and surface thermocouples until readings equalize at T_0 = 85.0 °C for 10 minutes.
Set cooling bath propeller speed to 800 RPM to establish high convective crossflow; verify bath temperature is stable at T_inf = 20.0 °C.
Trigger the pneumatic transfer arm to plunge the hot specimen instantaneously into the center of the agitated quench bath, synchronizing data logger t = 0.
Log centerline temperature T(t) continuously at 10 Hz over 60 seconds of cooling; compute temperature excess θ(t) = T(t) - T_inf.
Compare centerline and surface thermocouple readings to confirm temperature difference < 0.5 °C, verifying Biot number Bi < 0.1 validity.
Compute ln(θ/θ_0) at t = 10, 20, 30, 40, 50, and 60 s, plot ln(θ/θ_0) versus time t, and fit a linear regression to evaluate k_rate.
Points are your recorded observations. The solid regression line validates Transient Lumped Capacitance mathematical scaling.
| # | Cooling Elapsed Time t (s) | Log Dimensionless Temp ln(θ/θ_0) (ratio) | Quenching elapsed time t (s) | Log dimensionless temperature ln(θ/θ_0) | Remove |
|---|
No readings yet. Execute a process trial and record it.
In chemical process engineering, metallurgical heat treatment, polymer extrusion pelletizing, and food blanching, unsteady-state (transient) heat transfer dictates processing cycle times, microstructure evolution, and thermal stress generation. When a hot solid body is abruptly plunged into a cooler agitated fluid medium, heat conducts from the interior of the solid to its surface and is subsequently removed by convective boundary layer dissipation into the surrounding fluid. The governing thermal behavior depends critically on the relative magnitude of internal conduction resistance to external surface convective resistance, quantified by the dimensionless Biot number: Bi = h · L_c / k, where h is the convective heat transfer coefficient, k is solid thermal conductivity, and L_c = V / A_s is the characteristic body dimension. When Bi < 0.1, internal conductive resistance is negligible compared to surface convection, meaning temperature gradients within the solid remain virtually flat (spatially uniform temperature). Under this lumped thermal capacitance condition, the transient energy balance yields pure exponential decay: (T(t) - T_inf) / (T_0 - T_inf) = exp(-t / τ), where thermal time constant τ = (ρ · V · c_p) / (h · A_s) = 1 / k_rate. In this laboratory investigation, a brass test cylinder instrumented with centerline thermocouples is quenched from 85.0 °C into an agitated cooling bath to confirm lumped capacitance dynamics and evaluate the cooling decay rate k_rate.
Evaluated using a solid brass cylinder (diameter D = 25.0 mm, length L = 50.0 mm, density ρ = 8530 kg/m^3, specific heat c_p = 380 J/(kg·K), thermal conductivity k = 115 W/(m·K), Bi = 0.025). Linear regression models ln(θ/θ_0) versus t to extract k_rate = 0.0320 s^-1.