BMW · Working Student · Apr 2023 – Mar 2024

NVH Test Bench for Refrigerant Hose Characterisation

Designed a third-generation inertial measurement bench achieving a first resonance of 8,500 Hz — 3× better than the previous concept — enabling accurate characterisation of dynamic stiffness in composite refrigerant hoses for BMW's Neue Klasse electric vehicle platform.

Test bench in BMW laboratory

Third-generation inertial test bench — designed entirely in CATIA, manufactured in the BMW workshop

Background

In electric vehicles, the absence of internal combustion engine noise makes previously masked sounds clearly audible. Among these, vibrations from the A/C compressor transmitted through refrigerant hoses and rubber mounts into the cabin are a significant NVH challenge.

Car scheme
Vibration transmission path in an electric vehicle — compressor excitation travels through rubber mounts and refrigerant hoses directly into the passenger cabin

To optimize the packaging and design of these interface components (refrigerant hoses, rubber mounts), our vehicle integration strategy relied on predictive FEM simulations. However, these simulations were unreliable because they lacked accurate input data for the frequency-dependent dynamic stiffness of the components across four degrees of freedom: tension/compression, shear, torsion, and bending:

Tension/Compression degree of freedom Shear degree of freedom Torsion degree of freedom Bending degree of freedom
Four degrees of freedom characterised: longitudinal, shear, torsion, and bending — visualised using Direct Frequency Response simulations I built in Simcenter 3D (Nastran)

The problem was that no suitable measurement method existed. Standard test machines — designed for stiffer engine mounts — operated at the wrong force amplitudes and frequency ranges for the soft composite hoses in question (PTFE core, elastomer braid, textile sleeve). They also lacked the ability to measure rotational degrees of freedom, capturing only translational stiffness. The team had begun developing a dedicated test bench from scratch, and I joined the project at the prototype stage.

Methodology

The test bench uses an inertial measurement principle. A hose specimen is mounted between two metal parts: an outer active part driven by two electrodynamic shakers, and an inner passive part that floats freely. Accelerometers on both parts capture their motion; double integration of the signals yields displacement, and their difference gives the specimen deformation. Since the passive part is free-floating, the force through the hose is simply its mass multiplied by the measured acceleration — no multi-axis load cells required.

The symmetrical design enables all four loading modes through simple reconfiguration. When both shakers move in phase, the specimen sees pure tension/compression; reversing one shaker's phase produces bending. Rotating the rig 90° and repeating these two configurations yields torsion and shear. Center-of-gravity alignment along the hose axis eliminates cross-coupling, ensuring each mode is excited in isolation.

Tension/Compression test setup Bending test setup Torsion test setup Shear test setup
Extremely simplified model of the previous test rig generation that I build and simulated in Simcenter 3D purely to demonstrate the measurement principle — select a tab to see each degree of freedom configuration.

The Problem

The first-generation test bench worked as a proof of concept, but with a critical limitation. At lower frequencies the measured dynamic stiffness matched theoretical expectations, but beyond roughly 300–400 Hz the values skyrocketed exponentially — behaviour that does not reflect real elastomer physics. Feeding these artificially inflated results into the simulation would mean garbage in, garbage out: over-engineered mounts and hose geometries designed to solve problems that don't actually exist in the vehicle.

Expected vs measured result
Dynamic stiffness measured by the previous generation test bench (red) diverges exponentially from real elastomer behaviour (dashed) above 300 Hz

The root cause was structural resonance of the rig itself. The measurement principle assumes both metal parts behave as rigid bodies, and at low frequencies they do. But as the excitation frequency increases, the shakers begin exciting the natural modes of the fixture's structural members, introducing parasitic deformation into the force path and corrupting the stiffness calculation.

Expected vs measured result
At higher frequencies, the fixture's own structural members begin to resonate — introducing parasitic deformation into the force path and corrupting the stiffness calculation. Simulated in Simcenter 3D.

Design Objective

Given these findings, the goal for the next-generation test bench was clear: achieve exceptional structural rigidity, pushing the first natural frequency well above the 1,000 Hz operational range to ensure that the rig's own resonances would not interfere with the measurements.

My Contribution

Within the first months I learned the inertial measurement principle, CATIA, and Simcenter LMS Test.Lab — all from brief introductions followed by independent practice.

When my supervisor's Gen-3 design concept reached 3,000–3,300 Hz first resonance (verified in Simcenter 3D / Nastran), he concluded it was near-optimal. I disagreed — and over five personal weekend days developed an independent concept.

My design achieved 7,500 Hz first resonance in simulation — later refined collaboratively to 8,500 Hz. The concept was manufactured and became the production bench.

Resonance frequency comparison chart
First resonance frequency across three test bench generations — my redesign (blue) raised it from 3,300 to 8,500 Hz

Scope of Work

NVH Messung
Bode plot of dynamic torsional stiffness for three refrigerant hose specimens, measured from 10 to 1000 Hz with Simcenter LMS Test.Lab. Dynamic torsional stiffness magnitude on top and loss angle on the bottom — stable, repeatable curves confirm measurement quality

Results & Impact

Tools & Skills

CATIA V5 Simcenter 3D / Nastran Simcenter LMS Test.Lab SCADAS DAQ MATLAB NVH / Structural Dynamics Modal Analysis Dynamic Stiffness Measurement Excel (advanced)
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