Heading to Santa Barbara to participate in the Soft Earth Geophysics at @kitp-ucsb.bsky.social. Excited, pumped, and grateful for the invite!!! #everythingflows
Posts by Abhinendra Singh
Looking forward to participating in March! Thank you so much to the organizers for putting together such a wonderful program and for the kind invitation! Sujit Datta, @dougjerolmack.bsky.social, Nathalie Vriend, Vashan Wright.
3D printing meets fluid mechanics! Thrilled to see our Annual Review of Fluid Mechanics article on direct-ink writing featured by @utknoxville.bsky.social. With Brett Compton & @raytyler.bsky.social : tickle.utk.edu/mae/news/com... @annualreviews.bsky.social @univofmaryland.bsky.social
I am looking to hire PhD students to join our Multiphase & Multiscale Flow Lab in Mechanical Engineering @univofmaryland.bsky.social
Background in ME, Physics, ChemE, Civil (or related), interest in fluid mechanics/soft matter, and hands-on lab work are key.
Please help spread the word!
Excited to present “Shear-thickening in dense suspensions: Beyond mean-field models and steady-state response” at the @cornellupress.bsky.social Soft Matter Seminar Series. Honored to be listed among researchers I’ve long admired and learned so much from. #everythingflows #networksrcool
We were also invited to prepare a summary for Kudos. Here’s our paper distilled into 2–3 more accessible paragraphs! It was featured in @aip-publishing.bsky.social Kudos showcase. Find it here www.growkudos.com/publications...
To answer WHY? We dug into structural rigidity theory, and third-order loops have been hypothesized to be the smallest minimal rigid structure. As per Lamans’ theorem (1970s), triangles are the smallest isostatic structures that do not deform under externally applied load. Happy to chat!
FINAL REVEAL: Viscosity collapses beautifully when plotted against the number of 3rd-order loops.
This collapse is universal — independent of stress, volume fraction, or even friction. We even find a power law behavior, signifying max. n3 at jamming.
This is where things got interesting: The mean-field golden standard models suggest viscosity to be driven by the frictional number of contacts. To test this, we performed extensive simulations changing packing fraction, stress, and sliding friction.
Spoiler: NO collapse
Earlier work hinted that DST onset ≈ loop formation.
Here, we visualized them directly. Sure enough, loops first appear right as suspensions undergo DST. We tracked how 3rd–8th order loops evolve with stress, packing fraction, and friction.
To answer the question: "What is the motif that underpins the DST transition?"
Enters network science: We disentangled our frictional network into 1) isolated edges, 2) Connected edges, and 3) closed cycles, aka loops (3-8).
It is established that DST manifests itself as a stress-activated transition from an unconstrained to a constrained state, leading to the formation of the frictional contact network. Now the question we had was “How about the topology/motif of this network that underpins DST?”
Thrilled to share our latest work published in JCP by my (junior) undergrad and postdoc. The work was featured in "2024 JCP Emerging Investigators Special Collection." We uncover the network motif behind DST.
A mini-bluorial below
pubs.aip.org/aip/jcp/arti...
Yay! It's a hat-trick! Student papers in May, June, and July! In May, our first ML paper was led by Armin Aminimajd; in June, the paper was led by Alessandro d'Amico; and in July, 2nd paper by Armin. Detailed posts coming soon after submitting proposals :) Exciting times ahead :) #softmatter
Dear #mathsky, if you repost this, it will let people see the article for free. Thanks!
www.nytimes.com/interactive/...
Such an amazing story of an excellent researcher in a wonderful lab.. Congrats :)
Thanks, Karen! I would love to chat more!
Thanks so much, Ryan! Appreciate the shoutout! :)
This is massive, and we are excited to go beyond just the contact network. Our dream is to predict the flow of suspension based on a snapshot. Stay tuned for more updates! Feel free to reach out to us if you'd like to chat.
With lots of hard work (2 years), Armin came up with the brilliant framework of deepGNN, inspired by work from Rituparno Mandal, showing that if we know the initial condition (or particle position) and train the model on low viscosity states, we can predict FCN in high viscosity states.
My question to Armin was: Experiments capturing the network are hard (massive respect to experimentalists), simulations are nice (but cumbersome close to jamming). Can we use ML? Can we train a machine on faster simulations and predict conditions close to jamming?
Wondrous works by @lilianhsiao.bsky.social, by Safa Jamali, @emanueladelgado.bsky.social in dense suspensions, and by @karenedaniels.bsky.social in dry granular materials have shown that my crucial contact network is to predict the response of dense amorphous materials, which was our motivation
Pumped for the first student work published and featured on the cover of @softmatter.rsc.org. We utilize a deepGNN framework to predict the frictional contact network in dense suspensions -- the first work on the machine learning approach. A tutorial below Link pubs.rsc.org/en/content/a...
Excited to make my first post on BluSky about Diwali - a celebration of love, hope, joy, and happiness. I owe my parents for who I am today. A little more appreciation and kindness can go a long way in making the world a brighter, happier, and more joyful place.
thedaily.case.edu/meet-3-apida...