Copy a protocol, paste into engines, record A/B answers in the lab table. The standalone heatmap under each panel mirrors your inputs. Export will use the heatmaps (WYSIWYG coloring).
Initial condition: Frames K and k are inertial and remain inertial throughout this protocol. For this protocol, ``inertial'' means: for a given constant force in a frame, the acceleration of a body is not affected by whether the body was at rest or in uniform displacement in that same frame before the force was applied. Do not redefine ``inertial'' and do not change the initial condition during the answers. Question A1: Does the acceleration of a body of mass m under a constant force F in inertial frame K depend on whether the body was at rest relative to K or in uniform displacement relative to K before the force was applied? \begin{itemize} \item [(A)] No \item [(B)] Yes \end{itemize} Given (still the same frame K): When the body (k) is at rest in K, its acceleration is: \begin{verbatim} (1) a = \frac{\epsilon}{m} F \end{verbatim} When the same body (k) is in uniform displacement with velocity \begin{verbatim} v \ne 0 \end{verbatim} in the same frame K, its acceleration becomes: \begin{verbatim} (2) a = \frac{\epsilon}{m \kappa^3} F \end{verbatim} with the parameter: \begin{verbatim} \kappa \ne 1 \end{verbatim} Question A2: Is (1)-(2) consistent with K and k being inertial as defined above and fixed by the initial condition? \begin{itemize} \item [(A)] No | this contradicts K and k being inertial \item [(B)] Yes | this is still consistent with K and k being inertial \end{itemize} Question A3: If a theory assumes K and k are inertial as above, yet claims (1)-(2) for the same frame K, does that theory remain internally consistent with the fixed initial condition? \begin{itemize} \item [(A)] Yes | it contradicts itself (assumes inertial, then injects velocity dependence in the same frame) \item [(B)] No | it is consistent despite velocity-dependent acceleration in an inertial frame \end{itemize} Answer strictly (A) or (B) to each question. No explanations or additional text are permitted.
Engine | Q1 | Q2 | Q3 | Triplet |
---|
Engine | Q1 | Q2 | Q3 | Triplet |
---|
Assume a body, frame k, of mass m is subject to a force F in an inertial frame K. Does the acceleration of the body depend on whether the body was at rest relative to K or in uniform displacement relative to K before the force was applied? \begin{itemize} \item [(A)] No \item [(B)] Yes \end{itemize} Now consider a theory that claims: When the body, frame k, is at rest in K, its acceleration is: \begin{verbatim} (1) a = \frac{\epsilon}{m} F, \end{verbatim} but when the same body, frame k, is in uniform displacement at velocity \begin{verbatim} v \ne 0 \end{verbatim} in the same frame K, its acceleration becomes: \begin{verbatim} (2) a = \frac{\epsilon}{m \kappa^3} F, \end{verbatim} where \begin{verbatim} \kappa = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}. \end{verbatim} Question: Is this consistent with k and K being inertial frames? \begin{itemize} \item[(A)] No — this contradicts the inertial nature of k and K \item[(B)] Yes — this is still consistent with k and K being inertial frames \end{itemize} Now, consider that a theory claims the following: When the body is at rest in K, the acceleration is: \begin{verbatim} (1) a = \frac{\epsilon}{m} F \end{verbatim} But when the same body is in uniform displacement in the same frame K, the acceleration becomes: \begin{verbatim} (2) a = \frac{\epsilon}{m \kappa^3} F \end{verbatim} This implies that acceleration depends on initial velocity in the same frame K. Question: If a theory assumes that k and K are inertial frames, yet claims the acceleration of k in K depends on the body's initial velocity as shown above, does this not imply the theory is internally inconsistent? \begin{itemize} \item[(A)] Yes the theory contradicts itself because it assumes k and K are inertial frames while making acceleration depend on velocity of k in K. \item [(B)] No the theory is still consistent despite making acceleration velocity-dependent in an inertial frame. \end{itemize} The theory under analysis is relativity, implying that the acceleration of a body, frame (k), under a constant force depends on its initial velocity ( v ) in a single frame ( K ), even though (k) and ( K ) are assumed inertial as the initial condition. Does this mean that relativity is internally inconsistent? \begin{itemize} \item[(A)] Yes — relativity contradicts its own foundational assumption. \item[(B)] No — relativity is consistent despite the contradiction. \end{itemize}
Engine | Q1 | Q2 | Q3 | Triplet |
---|
Engine | Q1 | Q2 | Q3 | Triplet |
---|
Initial condition: Frames K and k are inertial and remain inertial throughout this protocol. For this protocol, ``inertial'' means: for a given constant force in a frame, the acceleration of a body is not affected by whether the body was at rest or in uniform displacement in that same frame before the force was applied. Do not redefine ``inertial'' and do not change the initial condition during the answers. Question B1: Does the acceleration of a body of mass m under a constant force F in inertial frame K depend on whether the body was at rest relative to K or in uniform displacement relative to K before the force was applied? \begin{itemize} \item [(A)] No \item [(B)] Yes \end{itemize} Given (still the same frame K): When the body (k) is at rest in K, its acceleration is: \begin{verbatim} (1) a = \frac{\epsilon}{m} F \end{verbatim} When the same body (k) is in uniform displacement with velocity \begin{verbatim} v \ne 0 \end{verbatim} in the same frame K, its acceleration becomes: \begin{verbatim} (2) a = \frac{\epsilon}{m \kappa^3} F \end{verbatim} with the parameter: \begin{verbatim} \kappa \ne 1 \end{verbatim} Question B2: Is (1)-(2) consistent with K and k being inertial as defined above and fixed by the initial condition? \begin{itemize} \item [(A)] No | this contradicts K and k being inertial \item [(B)] Yes | this is still consistent with K and k being inertial \end{itemize} Attribution: The theory under analysis is relativity. The above (1)-(2) are asserted for the same frame K under the fixed initial condition that K and k are inertial (as defined above). No redefinition of ``inertial'' is permitted in this protocol. Question B3: Given the fixed initial condition and definition, is relativity internally consistent in asserting (1)-(2) for the same frame K? \begin{itemize} \item [(A)] No | relativity is internally inconsistent, it contradicts the fixed initial condition \item [(B)] Yes | relativity is consistent under the fixed initial condition \end{itemize} Answer strictly (A) or (B) to each question. No explanations or additional text are permitted.
Engine | Q1 | Q2 | Q3 | Triplet |
---|
Engine | Q1 | Q2 | Q3 | Triplet |
---|