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Vector-Valued Function Calculus · Tutorial 792 of 999

Initial Conditions and Integration Constants for Vector Functions

Use a specified value of a vector function to determine the integration constant vector, then verify both the derivative and the given condition.

Advanced 9 min read

What You'll Learn

  • Write an antiderivative of a vector function component by component.
  • Distinguish a constant vector from a single scalar integration constant.
  • Use a specified vector value to solve for every component of the constant vector.
  • Justify why the initial value determines a unique antiderivative on an interval.
  • Check a result by differentiating it and substituting the specified input.
  • Identify errors caused by omitting or misapplying integration constants.

Why an Initial Value Determines the Constant

Integrating a vector function produces a family of antiderivatives. Each member of that family has the same derivative, because adding a constant vector does not change any component’s derivative. A specified value of the function at one input selects exactly one member of the family.

The calculation is component by component, but the condition is a vector equation: every component of the antiderivative must match the corresponding component of the specified vector at the specified input.

Key idea: If \(\mathbf{F}'(t)=\mathbf{f}(t)\) and \(\mathbf{F}(t_0)=\mathbf{v}_0\), then the integration constant vector is found by evaluating a general antiderivative at \(t_0\) and setting the result equal to \(\mathbf{v}_0\).

Definitions and the Constant-Vector Form

Let \(\mathbf{f}(t)=\langle f_1(t),f_2(t),\ldots,f_n(t)\rangle\) be a vector-valued function on an interval. An antiderivative of \(\mathbf{f}\) is a vector-valued function \(\mathbf{F}\) satisfying \(\mathbf{F}'(t)=\mathbf{f}(t)\) throughout that interval. Differentiation and integration of vector functions are defined component by component.

Definition: A constant vector is a vector \(\mathbf{C}=\langle C_1,C_2,\ldots,C_n\rangle\) whose components are constants. If \(\mathbf{F}\) is an antiderivative of \(\mathbf{f}\), then \(\mathbf{F}+\mathbf{C}\) is also an antiderivative of \(\mathbf{f}\).

The componentwise form of an indefinite integral is therefore

$$ \int \mathbf{f}(t)\,dt = \left\langle \int f_1(t)\,dt,\, \int f_2(t)\,dt,\, \ldots,\, \int f_n(t)\,dt \right\rangle +\mathbf{C}. $$

The constants \(C_1,\ldots,C_n\) are independent: the condition on one component does not require its constant to equal the constant in another component. Writing just one scalar \(C\) for the whole vector can wrongly force all components to share the same value.

An initial condition for a vector function specifies both an input \(t_0\) and a vector value \(\mathbf{v}_0\). The condition \(\mathbf{F}(t_0)=\mathbf{v}_0\) means that each component of \(\mathbf{F}(t_0)\) equals the corresponding component of \(\mathbf{v}_0\).

A Reliable Calculation Process

1
Integrate each component.
Write a separate constant for each component, or use a constant vector \(\mathbf{C}\).
2
Evaluate at the specified input.
Substitute \(t=t_0\) into every component of the general antiderivative.
3
Match the specified vector.
Set corresponding components equal and solve for each constant.
4
Check both requirements.
Differentiate the result and substitute \(t_0\) to confirm the derivative and the initial value.

The specified input need not be zero. In particular, do not set the constants equal to the given vector automatically: first evaluate the nonconstant parts of the antiderivative at the specified input.

Worked Examples

Worked Example: Determine a Constant Vector at Zero

Find \(\mathbf{F}(t)\) if \(\mathbf{F}'(t)=\langle 6t-2,\cos t\rangle\) and \(\mathbf{F}(0)=\langle 4,-1\rangle\).

Integrate each component:

$$ \mathbf{F}(t) = \langle 3t^2-2t+C_1,\ \sin t+C_2\rangle. $$

Apply the condition at \(t=0\). Since \(3(0)^2-2(0)=0\) and \(\sin 0=0\),

$$ \mathbf{F}(0) = \langle C_1,C_2\rangle = \langle 4,-1\rangle. $$

Matching components gives \(C_1=4\) and \(C_2=-1\). Thus

$$ \mathbf{F}(t)=\langle 3t^2-2t+4,\ \sin t-1\rangle. $$

Check the derivative: \(\mathbf{F}'(t)=\langle 6t-2,\cos t\rangle\). Check the condition: \(\mathbf{F}(0)=\langle 4,-1\rangle\). Both requirements hold.

Worked Example: Determine Constants at a Nonzero Input

Find \(\mathbf{G}(x)\) if \(\mathbf{G}'(x)=\langle e^x,4x^3\rangle\) and \(\mathbf{G}(\ln 2)=\langle 5,3\rangle\).

Integrating component by component gives

$$ \mathbf{G}(x)=\langle e^x+C_1,\ x^4+C_2\rangle. $$

At \(x=\ln 2\), use \(e^{\ln 2}=2\). The first component condition is \(2+C_1=5\), so \(C_1=3\). The second component condition is \((\ln 2)^4+C_2=3\), so \(C_2=3-(\ln 2)^4\). Therefore,

$$ \mathbf{G}(x) = \left\langle e^x+3,\ x^4+3-(\ln 2)^4 \right\rangle. $$

Differentiate to check: \(\mathbf{G}'(x)=\langle e^x,4x^3\rangle\). Now substitute \(x=\ln 2\): the first component is \(2+3=5\), and the second is \((\ln 2)^4+3-(\ln 2)^4=3\). Hence \(\mathbf{G}(\ln 2)=\langle 5,3\rangle\), as required.

Worked Example: Find Three Independent Constants

Find \(\mathbf{H}(t)\) if \(\mathbf{H}'(t)=\langle 2t,3t^2-4,\cos t\rangle\) and \(\mathbf{H}(2)=\langle 1,0,-3\rangle\).

An antiderivative with all three constants included is

$$ \mathbf{H}(t) = \langle t^2+C_1,\ t^3-4t+C_2,\ \sin t+C_3\rangle. $$

Evaluate each component at \(t=2\): \(2^2+C_1=4+C_1\), \(2^3-4(2)+C_2=8-8+C_2=C_2\), and \(\sin 2+C_3\). Set these equal to the specified components:

$$ 4+C_1=1,\qquad C_2=0,\qquad \sin 2+C_3=-3. $$

Thus \(C_1=-3\), \(C_2=0\), and \(C_3=-3-\sin 2\). The result is

$$ \mathbf{H}(t) = \langle t^2-3,\ t^3-4t,\ \sin t-3-\sin 2\rangle. $$

Differentiating gives \(\mathbf{H}'(t)=\langle 2t,3t^2-4,\cos t\rangle\). At \(t=2\), the components are \(4-3=1\), \(8-8=0\), and \(\sin 2-3-\sin 2=-3\). The derivative and the specified value both check.

Why the Initial Value Determines a Unique Antiderivative

The constant-vector rule is more than a convenient way to organize a calculation. On an interval, two antiderivatives of the same vector function can differ only by a constant vector. Here is the justification.

1
Compare two antiderivatives.
Suppose \(\mathbf{F}'(t)=\mathbf{f}(t)\) and \(\mathbf{G}'(t)=\mathbf{f}(t)\) on an interval \(I\). Define \(\mathbf{D}(t)=\mathbf{F}(t)-\mathbf{G}(t)\). By linearity of differentiation, \(\mathbf{D}'(t)=\mathbf{0}\).
2
Use the scalar zero-derivative result on each component.
Each component \(D_i(t)=F_i(t)-G_i(t)\) has derivative zero throughout \(I\). For any \(a,b\in I\), the Mean Value Theorem applied between them implies \(D_i(a)=D_i(b)\), so \(D_i\) is constant on \(I\).
3
Combine the component conclusions.
Every component of \(\mathbf{D}\) is constant, so \(\mathbf{F}(t)-\mathbf{G}(t)=\mathbf{C}\) for a constant vector \(\mathbf{C}\). Thus antiderivatives differ by a constant vector.
4
Apply the initial value.
If both antiderivatives satisfy \(\mathbf{F}(t_0)=\mathbf{v}_0\) and \(\mathbf{G}(t_0)=\mathbf{v}_0\), then \(\mathbf{C}=\mathbf{F}(t_0)-\mathbf{G}(t_0)=\mathbf{0}\). Therefore \(\mathbf{F}=\mathbf{G}\) throughout \(I\).

This argument requires the functions to be defined on an interval, so that any two inputs can be joined within the domain. It explains why one vector condition fixes all the constants and leaves only one antiderivative satisfying that condition.

A Common Mistake: Treating the Constant as One Scalar

Suppose an antiderivative has two components. A tempting but incorrect step is to write a single scalar constant in both:

$$ \int \langle 2t,3\rangle\,dt \ \overset{\text{wrong}}{=}\ \langle t^2+C,\ 3t+C\rangle. $$

This forces the two independent component constants to be equal. For instance, if the condition is \(\mathbf{F}(0)=\langle 1,5\rangle\), the first component requires \(C=1\), while the second requires \(C=5\). The resulting contradiction is caused by the incorrect shared constant, not by the condition.

The correction is to use two constants:

$$ \mathbf{F}(t)=\langle t^2+C_1,\ 3t+C_2\rangle. $$

Then \(\mathbf{F}(0)=\langle C_1,C_2\rangle=\langle 1,5\rangle\), so \(C_1=1\) and \(C_2=5\). The corrected function is \(\langle t^2+1,3t+5\rangle\). Its derivative is \(\langle 2t,3\rangle\), and its value at zero is \(\langle 1,5\rangle\).

Verification Is Part of the Solution

A computed constant vector should be checked in two different ways. Differentiating verifies that the function is an antiderivative of the stated vector function. Substituting the specified input verifies that it satisfies the stated value. Either check alone is incomplete: the right derivative does not guarantee the right initial value, and the right value at one input does not guarantee the right derivative elsewhere.

Takeaway: Integrate each component, retain an independent constant for each component, use the vector condition to solve for those constants, and check both the derivative and the specified value.

Check Your Understanding

For each question, show the component equations used to determine the constants. Check your results by differentiating and substituting the given input.

  1. Find \(\mathbf{P}(t)\) if \(\mathbf{P}'(t)=\langle 4t,2\rangle\) and \(\mathbf{P}(1)=\langle 3,-1\rangle\).
  2. Why must a vector antiderivative include independent constants for its different components?
  3. Find \(\mathbf{Q}(x)\) if \(\mathbf{Q}'(x)=\langle \cos x,6x^2\rangle\) and \(\mathbf{Q}(0)=\langle 2,4\rangle\).
  4. What condition on the domain is used in the uniqueness justification, and where does it enter?
  5. A student writes \(\langle t^2+C,5t+C\rangle\) as a general antiderivative of \(\langle 2t,5\rangle\). Explain what is wrong and write the correct general form.

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