Math Problem Statement

S1theta2_dot(d4*(S2S3 - C2C3) + S2a2) - theta1_dot(C1a1 + S1d3 + d4*(C1C2S3 + C1C3S2) + C1C2a2) + S1d4theta3_dot*(S2S3 - C2C3) đơn giản biểu thức này

Solution

To simplify the given expression:

S1θ˙2(d4(S2S3C2C3)+S2a2)θ˙1(C1a1+S1d3+d4(C1C2S3+C1C3S2)+C1C2a2)+S1d4θ˙3(S2S3C2C3)S_1 \cdot \dot{\theta}_2 \left( d_4 \left( S_2 S_3 - C_2 C_3 \right) + S_2 a_2 \right) - \dot{\theta}_1 \left( C_1 a_1 + S_1 d_3 + d_4 \left( C_1 C_2 S_3 + C_1 C_3 S_2 \right) + C_1 C_2 a_2 \right) + S_1 d_4 \dot{\theta}_3 \left( S_2 S_3 - C_2 C_3 \right)

We can begin by looking for common terms and factoring them out where possible. For this purpose, let's label components to organize our approach:

  • S1,S2,S3,C1,C2,C3S_1, S_2, S_3, C_1, C_2, C_3 are likely trigonometric functions (sine and cosine of angles).
  • a1,a2,d3,d4a_1, a_2, d_3, d_4 appear to be constants or parameters.
  • θ˙1,θ˙2,θ˙3\dot{\theta}_1, \dot{\theta}_2, \dot{\theta}_3 are derivatives with respect to time, typically angular velocities.

Step-by-Step Simplification:

  1. Group terms involving S1θ˙2S_1 \cdot \dot{\theta}_2: S1θ˙2(d4(S2S3C2C3)+S2a2)S_1 \cdot \dot{\theta}_2 \left( d_4 \left( S_2 S_3 - C_2 C_3 \right) + S_2 a_2 \right)

  2. Group terms involving θ˙1-\dot{\theta}_1: θ˙1(C1a1+S1d3+d4(C1C2S3+C1C3S2)+C1C2a2)-\dot{\theta}_1 \left( C_1 a_1 + S_1 d_3 + d_4 \left( C_1 C_2 S_3 + C_1 C_3 S_2 \right) + C_1 C_2 a_2 \right)

  3. Group terms involving S1d4θ˙3S_1 d_4 \dot{\theta}_3: S1d4θ˙3(S2S3C2C3)S_1 d_4 \dot{\theta}_3 \left( S_2 S_3 - C_2 C_3 \right)

Factor Common Expressions:

  • You have the common factor (S2S3C2C3)(S_2 S_3 - C_2 C_3) in several places. Factor it out from the terms where it appears: (S2S3C2C3)(S1θ˙2d4+S1d4θ˙3)(S_2 S_3 - C_2 C_3) \left( S_1 \dot{\theta}_2 d_4 + S_1 d_4 \dot{\theta}_3 \right) This simplifies to: S1d4(θ˙2+θ˙3)(S2S3C2C3)S_1 d_4 \left( \dot{\theta}_2 + \dot{\theta}_3 \right) (S_2 S_3 - C_2 C_3)
  1. Simplify the remaining terms: The remaining part of the expression is: θ˙1(C1a1+S1d3+d4(C1C2S3+C1C3S2)+C1C2a2)-\dot{\theta}_1 \left( C_1 a_1 + S_1 d_3 + d_4 \left( C_1 C_2 S_3 + C_1 C_3 S_2 \right) + C_1 C_2 a_2 \right) This term doesn't have a common factor across all parts, so it stays as is.

Final Expression:

Thus, the simplified version of the original expression is:

S1d4(θ˙2+θ˙3)(S2S3C2C3)θ˙1(C1a1+S1d3+d4(C1C2S3+C1C3S2)+C1C2a2)S_1 d_4 \left( \dot{\theta}_2 + \dot{\theta}_3 \right) (S_2 S_3 - C_2 C_3) - \dot{\theta}_1 \left( C_1 a_1 + S_1 d_3 + d_4 \left( C_1 C_2 S_3 + C_1 C_3 S_2 \right) + C_1 C_2 a_2 \right)

Let me know if you'd like further clarification or additional steps.


Additional Related Questions:

  1. How do trigonometric functions like sine and cosine affect the simplification of terms in this kind of expression?
  2. What are some physical interpretations of terms like S1,S2,S3,C1,C2,C3S_1, S_2, S_3, C_1, C_2, C_3 in the context of robotics or kinematics?
  3. What is the significance of the derivative terms (θ˙1,θ˙2,θ˙3\dot{\theta}_1, \dot{\theta}_2, \dot{\theta}_3) in the expression?
  4. How would you apply this simplified expression in real-world simulations or calculations?
  5. How can you use this expression to determine angular velocities in a robotic arm?

Tip: When simplifying expressions involving trigonometric terms, look for common factors like S2S3C2C3S_2 S_3 - C_2 C_3, which can drastically reduce complexity.

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Math Problem Analysis

Mathematical Concepts

Algebra
Trigonometry
Symbolic Computation

Formulas

Trigonometric identities: sin(A ± B) = sin A cos B ± cos A sin B
Factoring common terms in algebraic expressions

Theorems

Trigonometric simplification rules
Algebraic factoring principles

Suitable Grade Level

University (Engineering, Robotics, or Mathematics)