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Prove the product rule for the dot product of vector functions: d/dt(U · V) = U · dV/dt + dU/dt · V

Mathematics

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To show the product rule for the dot product of vector functions, we will start by defining the given vectors and then compute both sides of the identity ddt(U⃗⋅V⃗)=U⃗⋅dV⃗dt+dU⃗dt⋅V⃗\frac{d}{dt}(\vec{U} \cdot \vec{V}) = \vec{U} \cdot \frac{d\vec{V}}{dt} + \frac{d\vec{U}}{dt} \cdot \vec{V}.

  1. Define the given vectors.

    The vectors U⃗\vec{U} and V⃗\vec{V} are given as:

    U⃗=F1(t)i⃗+g1(t)j⃗+h1(t)k⃗\vec{U} = F_1(t)\vec{i} + g_1(t)\vec{j} + h_1(t)\vec{k} V⃗=F2(t)i⃗+g2(t)j⃗+h2(t)k⃗\vec{V} = F_2(t)\vec{i} + g_2(t)\vec{j} + h_2(t)\vec{k}
  2. Calculate the dot product U⃗⋅V⃗\vec{U} \cdot \vec{V}.

    The dot product of two vectors is the sum of the products of their corresponding components:

    U⃗⋅V⃗=F1(t)F2(t)+g1(t)g2(t)+h1(t)h2(t)\vec{U} \cdot \vec{V} = F_1(t)F_2(t) + g_1(t)g_2(t) + h_1(t)h_2(t)
  3. Differentiate U⃗⋅V⃗\vec{U} \cdot \vec{V} with respect to tt.

    We apply the product rule for scalar functions to each term:

    ddt(U⃗⋅V⃗)=ddt(F1(t)F2(t))+ddt(g1(t)g2(t))+ddt(h1(t)h2(t))\frac{d}{dt}(\vec{U} \cdot \vec{V}) = \frac{d}{dt}(F_1(t)F_2(t)) + \frac{d}{dt}(g_1(t)g_2(t)) + \frac{d}{dt}(h_1(t)h_2(t)) ddt(U⃗⋅V⃗)=(F1′(t)F2(t)+F1(t)F2′(t))+(g1′(t)g2(t)+g1(t)g2′(t))+(h1′(t)h2(t)+h1(t)h2′(t))\frac{d}{dt}(\vec{U} \cdot \vec{V}) = (F_1'(t)F_2(t) + F_1(t)F_2'(t)) + (g_1'(t)g_2(t) + g_1(t)g_2'(t)) + (h_1'(t)h_2(t) + h_1(t)h_2'(t))

    Rearranging the terms, we get:

    ddt(U⃗⋅V⃗)=(F1(t)F2′(t)+g1(t)g2′(t)+h1(t)h2′(t))+(F1′(t)F2(t)+g1′(t)g2(t)+h1′(t)h2(t))(1)\frac{d}{dt}(\vec{U} \cdot \vec{V}) = (F_1(t)F_2'(t) + g_1(t)g_2'(t) + h_1(t)h_2'(t)) + (F_1'(t)F_2(t) + g_1'(t)g_2(t) + h_1'(t)h_2(t)) \quad (1)
  4. Calculate the derivatives of the individual vectors, dU⃗dt\frac{d\vec{U}}{dt} and dV⃗dt\frac{d\vec{V}}{dt}.

    dU⃗dt=F1′(t)i⃗+g1′(t)j⃗+h1′(t)k⃗\frac{d\vec{U}}{dt} = F_1'(t)\vec{i} + g_1'(t)\vec{j} + h_1'(t)\vec{k} dV⃗dt=F2′(t)i⃗+g2′(t)j⃗+h2′(t)k⃗\frac{d\vec{V}}{dt} = F_2'(t)\vec{i} + g_2'(t)\vec{j} + h_2'(t)\vec{k}
  5. Calculate the right-hand side of the identity

    U⃗⋅dV⃗dt+dU⃗dt⋅V⃗\vec{U} \cdot \frac{d\vec{V}}{dt} + \frac{d\vec{U}}{dt} \cdot \vec{V}.
    First, calculate U⃗⋅dV⃗dt\vec{U} \cdot \frac{d\vec{V}}{dt}:

    U⃗⋅dV⃗dt=(F1(t)i⃗+g1(t)j⃗+h1(t)k⃗)⋅(F2′(t)i⃗+g2′(t)j⃗+h2′(t)k⃗)\vec{U} \cdot \frac{d\vec{V}}{dt} = (F_1(t)\vec{i} + g_1(t)\vec{j} + h_1(t)\vec{k}) \cdot (F_2'(t)\vec{i} + g_2'(t)\vec{j} + h_2'(t)\vec{k}) U⃗⋅dV⃗dt=F1(t)F2′(t)+g1(t)g2′(t)+h1(t)h2′(t)\vec{U} \cdot \frac{d\vec{V}}{dt} = F_1(t)F_2'(t) + g_1(t)g_2'(t) + h_1(t)h_2'(t)

    Next, calculate dU⃗dt⋅V⃗\frac{d\vec{U}}{dt} \cdot \vec{V}:

    dU⃗dt⋅V⃗=(F1′(t)i⃗+g1′(t)j⃗+h1′(t)k⃗)⋅(F2(t)i⃗+g2(t)j⃗+h2(t)k⃗)\frac{d\vec{U}}{dt} \cdot \vec{V} = (F_1'(t)\vec{i} + g_1'(t)\vec{j} + h_1'(t)\vec{k}) \cdot (F_2(t)\vec{i} + g_2(t)\vec{j} + h_2(t)\vec{k}) dU⃗dt⋅V⃗=F1′(t)F2(t)+g1′(t)g2(t)+h1′(t)h2(t)\frac{d\vec{U}}{dt} \cdot \vec{V} = F_1'(t)F_2(t) + g_1'(t)g_2(t) + h_1'(t)h_2(t)

    Now, sum these two results:

    U⃗⋅dV⃗dt+dU⃗dt⋅V⃗=(F1(t)F2′(t)+g1(t)g2′(t)+h1(t)h2′(t))+(F1′(t)F2(t)+g1′(t)g2(t)+h1′(t)h2(t))(2)\vec{U} \cdot \frac{d\vec{V}}{dt} + \frac{d\vec{U}}{dt} \cdot \vec{V} = (F_1(t)F_2'(t) + g_1(t)g_2'(t) + h_1(t)h_2'(t)) + (F_1'(t)F_2(t) + g_1'(t)g_2(t) + h_1'(t)h_2(t)) \quad (2)
  6. Compare the results from Step 3 and Step 5.

    Comparing equation (1) and equation (2), we see that both sides are identical.

    ddt(U⃗⋅V⃗)=U⃗⋅dV⃗dt+dU⃗dt⋅V⃗\boxed{\frac{d}{dt}(\vec{U} \cdot \vec{V}) = \vec{U} \cdot \frac{d\vec{V}}{dt} + \frac{d\vec{U}}{dt} \cdot \vec{V}}

    This shows the product rule for the dot product of vector functions.

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