A) Force is proportional to the square of the distance. B) Force is independent of the distance. C) Force scales linearly with distance. D) Force is inversely proportional to distance.
A) James Prescott Joule B) Robert Hooke C) Isaac Newton D) Albert Einstein
A) 1660 B) 1676 C) 1687 D) 1678
A) Fs = kx B) Fs = k + x C) Fs = x/k D) Fs = k/x
A) x B) m C) F D) k
A) Battery B) Transistor C) Capacitor D) Manometer
A) When forces exceed a certain limit. B) At very low temperatures. C) When the force is zero. D) When the distance is zero.
A) Einsteinian B) Pascalian C) Hookean D) Newtonian
A) The restoring force is opposite to the displacement. B) The spring constant is negative. C) The spring is losing energy. D) The force is reducing over time.
A) τ = θ/k B) τ = kθ² C) τ = k/θ D) τ = -kθ
A) Watts (W) B) Joules (J) C) Newton-meters (N·m) D) Newtons (N)
A) U = kx² B) U = 1/2kx² C) U = 1/2k/x² D) U = kx
A) f = (1/2π) * sqrt(k/m) B) f = 2π * sqrt(m/k) C) f = 2π * sqrt(k/m) D) f = (1/2π) * sqrt(m/k)
A) A second-order tensor B) A vector constant C) A fourth-order tensor D) A scalar constant
A) Steel B) Rubber C) Concrete D) Aluminum
A) A scalar value B) A fourth-order tensor C) A first-order tensor D) A second-order tensor
A) Meters (m) B) Newtons (N) C) Joules (J) D) Pascals (Pa)
A) The square of the stiffness tensor B) The inverse of the stiffness tensor C) The derivative of the stiffness tensor D) The sum of the stiffness tensor
A) 9 B) 5 C) 21 D) 3
A) Properties of rubber only B) Properties of isotropic materials C) Mass of a spring D) Temperature in a system |