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