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