Solve Applied Maths Urgent Probl. 1: 20 Marks

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SUMMARY

The discussion focuses on solving a complex applied mathematics problem involving Cartesian and polar coordinate systems. Participants analyze vectors v1 and v2 defined as v1 = −4ˆx + 0ˆy and v2 = 2ˆx − 7ˆy, and derive the corresponding polar unit vectors ˆr and ˆθ. Additionally, the motion of a particle is described by the position vector r(t) = αtxˆ + (βt² − t)ˆy, with the goal of expressing the velocity vector v(t) in terms of ˆr and ˆθ. The discussion emphasizes the differentiation of r(t) to obtain the velocity vector in Cartesian coordinates and its conversion into polar coordinates.

PREREQUISITES
  • Understanding of Cartesian and polar coordinate systems
  • Knowledge of vector calculus and differentiation
  • Familiarity with unit vectors ˆx, ˆy, ˆr, and ˆθ
  • Ability to perform linear combinations of vectors
NEXT STEPS
  • Learn how to derive polar coordinate unit vectors from Cartesian coordinates
  • Study the process of differentiating vector functions with respect to time
  • Explore the application of linear combinations in vector analysis
  • Investigate the relationship between Cartesian and polar representations of motion
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Students and professionals in applied mathematics, physics, and engineering who are working on vector analysis and motion in different coordinate systems.

bilal98732
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Problem 1 20 marks (i) ˆx = (1, 0) and ˆy = (0, 1) are the Cartesian unit vectors and the vectors v1 and v2 are defined as v1 = −4ˆx + 0ˆy , v2 = 2ˆx − 7ˆy . Determine the polar coordinate unit vectors ˆr and ˆθ for v1 and v2 and hence express v1 and v2 as a linear combination of ˆr and ˆθ. [4]

(ii) A particle’s motion is described by the following position vector r(t) = αtxˆ + (βt2 − t)ˆy Determine the polar coordinate unit vectors ˆr and ˆθ for r. [4]

(iii) By differentiating with respect to time r(t), given in (ii) show that the velocity vector written in a Cartesian basis for this particle is v(t) = αxˆ + (2βt − 1)ˆy . [2] (iv) Using the ˆr and ˆθ you found in (ii) above, write v(t) as a linear combination of rˆ and ˆθ. [4]

(v) Differentiate the expression for r(t) you got in part (ii) (in terms of ˆr and ˆθ, and using the expressions ˙rˆ = ˙θ ˆθ , ˙ˆθ = − ˙θrˆ derived in the lectures, show that you obtain the same answer as in part (iv) [6]where r(vector) = r modulus * r
r^ = cos(pheta)x + sin(pheta)y
pheta^ = -sin(pheta)x +cos(pheta)yi am able to do i) and ii) but unbale to expres v(t) in terms of r and pheta
 
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bilal98732 said:
Problem 1 20 marks (i) ˆx = (1, 0) and ˆy = (0, 1) are the Cartesian unit vectors and the vectors v1 and v2 are defined as v1 = −4ˆx + 0ˆy , v2 = 2ˆx − 7ˆy . Determine the polar coordinate unit vectors ˆr and ˆθ for v1 and v2 and hence express v1 and v2 as a linear combination of ˆr and ˆθ. [4]

(ii) A particle’s motion is described by the following position vector r(t) = αtxˆ + (βt2 − t)ˆy Determine the polar coordinate unit vectors ˆr and ˆθ for r. [4]
What did you get for the position vector?
What do you get when you take the time derivative of that expression?
 

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