Search Results

Lesson 11, part 3: obtaining the Wagner damping function

Lesson 11, part 3: obtaining the Wagner damping function

Lesson 11, part 2: making Maxwell non-linear - the Wagner damping function

Lesson 11, part 2: making Maxwell non-linear - the Wagner damping function

Lesson 11, part 1: multimode integral Maxwell

Lesson 11, part 1: multimode integral Maxwell

Lesson 12, part 3: the presence of normal stresses in shear flow for the UCM equation

Lesson 12, part 3: the presence of normal stresses in shear flow for the UCM equation

Lesson 9, part 1: an introduction to the differential Maxwell model for viscoelasticity

Lesson 9, part 1: an introduction to the differential Maxwell model for viscoelasticity

Lesson 9, part 2: the steady shear and stress relaxation response of differential Maxwell

Lesson 9, part 2: the steady shear and stress relaxation response of differential Maxwell

Lesson 9, part 3: oscillatory response of differential Maxwell

Lesson 9, part 3: oscillatory response of differential Maxwell

ADIW02 | Prof. Jorn Dunkel | Spontaneous chiral symmetry breaking in higher-order PDE models of...

ADIW02 | Prof. Jorn Dunkel | Spontaneous chiral symmetry breaking in higher-order PDE models of...

Gas extinguishing technology with inert gas - This is how it works

Gas extinguishing technology with inert gas - This is how it works

Lesson 7, part 4: analysis of rotational rheometry data

Lesson 7, part 4: analysis of rotational rheometry data

Rheology - introduction to Section C [presented by Dr Bart Hallmark, University of Cambridge]

Rheology - introduction to Section C [presented by Dr Bart Hallmark, University of Cambridge]

Lesson 12, part : convected constitutive equations and the Upper Convected Maxwell model

Lesson 12, part : convected constitutive equations and the Upper Convected Maxwell model