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