Search alternatives:
step decrease » sizes decrease (Expand Search), we decrease (Expand Search)
teer decrease » greater decrease (Expand Search)
a decrease » _ decrease (Expand Search), _ decreased (Expand Search), _ decreases (Expand Search)
step decrease » sizes decrease (Expand Search), we decrease (Expand Search)
teer decrease » greater decrease (Expand Search)
a decrease » _ decrease (Expand Search), _ decreased (Expand Search), _ decreases (Expand Search)
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2621
Scheme and results of orthogonal test.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2622
Effect of collision material on COR.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2623
Computational parameters used in the simulations.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2624
Collision materials.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2625
Diagram of displacement variation.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2626
Scheme and results of orthogonal test.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2627
The millet mode.
Published 2025“…A combination of bench and simulation tests validated the test results, showing no significant differences and confirming the method’s viability for determining COR. …”
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2628
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2629
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2630
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2631
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2632
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2633
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2634
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2635
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2636
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2637
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2638
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2639
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2640